astro-ph9910093.xml

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}^{'}

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

urfeld

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

field

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}^{'}

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

t_{0}

age

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

larger

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}^{'}

vacuum expectation value

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

a large rather than a small

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

scale parameter

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

a constant value

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

α_{g}

constant

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

α_{g}

constant

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

α_{g}

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

non-zero

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

R^{2} (t, α = 0, k < 0) = - 2 A / k ℏ c S_{0}^{2} - k c^{2} t^{2}

S_{0}

background field

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{k} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{M} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

the current era

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{M} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{M} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

negative

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

control

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

the current era

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

the same order of magnitude

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t)

future

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

the standard model

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

the current era

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{M} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{M} (t_{0})

era

1 \geq Ω_{k} (t_{0}) \geq 0

{\bar{Ω}}_{Λ} (t_{0})

the current era

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t_{0})

1 \geq Ω_{k} (t_{0}) \geq 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

t_{0}

age

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

α

parameter

α_{g}

constant

α

parameter

α_{g}

constant

α

parameter

α_{g}

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{k} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{k} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

future

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{V}

a large

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{m a x}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}^{'}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{V}

big or small

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{V}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

urfeld

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

field

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}^{'}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{m a x}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{m a x}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{k i n}^{μ ν}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{V}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{m a x}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T^{μ ν}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{m a x}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{V}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

larger

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{m a x}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{V}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{V}

(highest) critical temperature

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}^{'}

vacuum expectation value

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{m a x}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

a large rather than a small

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

scale parameter

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T^{μ ν}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

a constant value

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{m a x}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{V}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

non-zero

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{V}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{m a x}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{V}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{V}

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

T_{m a x}

the temperature

T_{m a x}^{2} \sim - k ℏ c S_{0}^{2} / 2 A

a maximum (negative curvature supported) temperature

S_{0}

background field

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

α = 0

α_{g}

constant

α = 0

α_{g}

constant

α = 0

α_{g}

R (t) \sim t

t_{0}

age

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

T_{V}

a large

T_{m a x}

T_{V}

a large

T_{m a x}

T_{V}

a large

T_{m a x}

T_{V}

a large

T_{k i n}^{μ ν}

T_{V}

a large

T_{m a x}

T_{V}

a large

T^{μ ν}

T_{V}

a large

T_{m a x}

T_{V}

a large

T^{μ ν}

the associated energy-momentum tensor

T_{V}

a large

T_{m a x}

T_{V}

a large

T_{m a x}

T_{V}

a large

T^{μ ν}

T_{V}

a large

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

a large

T_{m a x}

T_{V}

a large

V_{m i n}^{G L}

which

T_{V}

a large

T_{m a x}

T_{V}

a large

T_{m a x}

the temperature

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

q (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{k} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{k} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

q_{0}

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

q (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

q (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

t_{0}

age

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t)

future

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

q_{0}

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

q (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

q (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{M} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

q (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

small, negative

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

Λ = V_{m i n}^{G L}

vacuum energy density

L_{P L}^{- 1}

inverse Planck length

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

Λ = V_{m i n}^{G L}

vacuum energy density

G_{F}

Fermi’s

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

Λ = V_{m i n}^{G L}

vacuum energy density

L_{P L}^{- 1}

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

the cosmological

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

a small, negative

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

an appropriate

Λ = V_{m i n}^{G L}

vacuum energy density

G_{e f f}

t_{0} H (t_{0}) = a r c t a n h [{(- q (t_{0}))}^{1 / 2}] / {(- q (t_{0}))}^{1 / 2}

universe

q_{0}

t_{0} H (t_{0}) = a r c t a n h [{(- q (t_{0}))}^{1 / 2}] / {(- q (t_{0}))}^{1 / 2}

universe

q (t)

conformal cosmology

t_{0} H (t_{0}) = a r c t a n h [{(- q (t_{0}))}^{1 / 2}] / {(- q (t_{0}))}^{1 / 2}

universe

q (t)

t_{0} H (t_{0}) = a r c t a n h [{(- q (t_{0}))}^{1 / 2}] / {(- q (t_{0}))}^{1 / 2}

universe

q_{0}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{V}

a large

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{m a x}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}^{'}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{V}

big or small

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{V}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

urfeld

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

field

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}^{'}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{m a x}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{m a x}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{k i n}^{μ ν}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{V}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{m a x}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T^{μ ν}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{m a x}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{V}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T^{μ ν}

the associated energy-momentum tensor

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

larger

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{m a x}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{V}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{V}

(highest) critical temperature

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}^{'}

vacuum expectation value

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{m a x}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

a large rather than a small

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

scale parameter

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T^{μ ν}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

a constant value

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{m a x}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{V}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

V_{m i n}^{G L}

which

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

non-zero

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{V}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{m a x}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{V}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{V}

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

T_{m a x}

the temperature

- c ℏ λ S_{0}^{4} = σ T_{V}^{4}

S_{0}

background field

q (t_{0})

q_{0}

q (t_{0})

q (t)

conformal cosmology

q (t_{0})

q (t)

q (t_{0})

q_{0}

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

q (t_{0}) = 0

q_{0}

q (t_{0}) = 0

q (t)

conformal cosmology

q (t_{0}) = 0

q (t)

q (t_{0}) = 0

q_{0}

T_{m a x}

T_{V}

a large

T_{m a x}

T_{V}

big or small

T_{m a x}

T_{V}

T_{m a x}

T_{k i n}^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T_{V}

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

ρ_{M} (t)

perfectly normal

ρ_{M} (t_{0})

ρ_{M} (t)

perfectly normal

ρ_{M} (t_{0})

ρ_{M} (t)

perfectly normal

t_{0}

age

ρ_{M} (t)

perfectly normal

ρ_{M} (t_{0})

ρ_{M} (t)

perfectly normal

ρ_{M} (t_{0})

order

ρ_{M} (t)

perfectly normal

ρ_{M} (t_{0})

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{V}

a large

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{m a x}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

ρ_{M} (t_{0})

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{V}

big or small

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{V}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

ρ_{M} (t_{0})

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{m a x}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{m a x}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{k i n}^{μ ν}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{V}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{m a x}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T^{μ ν}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{m a x}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{V}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T^{μ ν}

the associated energy-momentum tensor

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

t_{0}

age

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{m a x}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{V}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{V}

(highest) critical temperature

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{m a x}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

ρ_{M} (t_{0})

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T^{μ ν}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{m a x}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

ρ_{M} (t_{0})

order

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{V}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

ρ_{M} (t_{0})

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{V}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{m a x}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{V}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{V}

ρ_{M} (t) = A / R^{4} = σ T^{4}

the complete family of solutions

T_{m a x}

the temperature

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T (t)

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T_{m a x} ≫ T (t_{0})

T_{V} ≫ T (t_{0})

T_{k i n}^{μ ν}

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T^{μ ν}

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T^{μ ν}

the associated energy-momentum tensor

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T_{m a x} ≫ T (t_{0})

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T^{μ ν}

T_{V} ≫ T (t_{0})

T_{m a x} ≫ T (t_{0})

T_{V} ≫ T (t_{0})

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

V_{m i n}^{G L}

which

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T_{m a x}

the temperature

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

urfeld

S_{0}^{'}

S_{0}

field

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

larger

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

a large rather than a small

S_{0}^{'}

S_{0}

scale parameter

S_{0}^{'}

S_{0}

a constant value

S_{0}^{'}

S_{0}

non-zero

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

background field

ρ_{M} (t_{0})

ρ_{M} (t)

perfectly normal

ρ_{M} (t_{0})

ρ_{M} (t)

ρ_{M} (t_{0})

ρ_{M} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

small, negative

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{F}

Fermi’s

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

the cosmological

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

a small, negative

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

an appropriate

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

G_{e f f}

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{Λ} (t)

G_{e f f}

small, negative

G_{F}

Fermi’s

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

α^{1 / 2} c t_{0}

the quantity

α_{g}

constant

α^{1 / 2} c t_{0}

the quantity

α_{g}

constant

α^{1 / 2} c t_{0}

the quantity

α_{g}

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{k} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{M} (t)

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{M} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

the current era

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{M} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{M} (t)

Ω_{k} (t)

Ω_{M} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

negative

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t)

control

Ω_{k} (t)

t_{0}

age

Ω_{k} (t)

Ω_{M} (t)

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

Ω_{M} (t)

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t)

future

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t)

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{M} (t)

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

Ω_{M} (t)

Ω_{k} (t)

Ω_{M} (t_{0})

the current era

Ω_{k} (t)

Ω_{M} (t)

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{k} (t_{0})

orders

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t)

G > 0

G_{e f f}

small, negative

G > 0

G_{e f f}

G > 0

G_{e f f}

G > 0

G_{e f f}

G > 0

G_{e f f}

G > 0

G_{e f f}

G > 0

G_{e f f}

G > 0

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G > 0

G_{e f f}

G > 0

G_{e f f}

G > 0

G_{e f f}

G > 0

G_{F}

Fermi’s

G > 0

G_{e f f}

G > 0

G_{e f f}

the cosmological

G > 0

G_{e f f}

a small, negative

G > 0

G_{e f f}

an appropriate

G > 0

G_{e f f}

T_{m a x} ≫ T_{V} ≫ T (t_{0})

T (t)

T_{m a x} ≫ T_{V} ≫ T (t_{0})

T_{k i n}^{μ ν}

T_{m a x} ≫ T_{V} ≫ T (t_{0})

T^{μ ν}

T_{m a x} ≫ T_{V} ≫ T (t_{0})

T^{μ ν}

the associated energy-momentum tensor

T_{m a x} ≫ T_{V} ≫ T (t_{0})

T^{μ ν}

T_{m a x} ≫ T_{V} ≫ T (t_{0})

V_{m i n}^{G L}

which

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{k} (t)

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

negative

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t)

control

Ω_{k} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t)

future

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{k} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t)

t_{0}

age

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

β = {(1 - 16 A λ / k^{2} ℏ c)}^{1 / 2}

parameters

β^{*}

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

T_{V}

big or small

T_{m a x}

T_{V}

big or small

T_{m a x}

T_{V}

big or small

T_{m a x}

T_{V}

big or small

T_{k i n}^{μ ν}

T_{V}

big or small

T_{m a x}

T_{V}

big or small

T^{μ ν}

T_{V}

big or small

T_{m a x}

T_{V}

big or small

T^{μ ν}

the associated energy-momentum tensor

T_{V}

big or small

T_{m a x}

T_{V}

big or small

T_{m a x}

T_{V}

big or small

T^{μ ν}

T_{V}

big or small

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

big or small

T_{m a x}

T_{V}

big or small

V_{m i n}^{G L}

which

T_{V}

big or small

T_{m a x}

T_{V}

big or small

T_{m a x}

the temperature

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t)

t_{0}

age

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t, α = 0, k < 0)

t_{0}

age

Ω_{Λ} (t, α = 0, k < 0)

α_{g}

constant

Ω_{Λ} (t, α = 0, k < 0)

α_{g}

constant

Ω_{Λ} (t, α = 0, k < 0)

α_{g}

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{k} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{k} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{M} (t)

future

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

the line

Ω_{Λ} (t)

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{k i n}^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

T_{V}

V_{m i n}^{G L}

which

T_{V}

T_{m a x}

T_{V}

T_{m a x}

the temperature

α

matter how large

α_{g}

constant

α

matter how large

α_{g}

constant

α

matter how large

α_{g}

S_{0}

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

S_{0}^{'}

vacuum expectation value

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

t_{0}

age

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

T (t)

T_{V}

a large

T (t)

T_{m a x}

T (t)

T_{V}

big or small

T (t)

T_{V}

T (t)

T_{m a x}

T (t)

T_{m a x}

T (t)

T_{k i n}^{μ ν}

T (t)

T (t_{0})

current temperature

T (t)

T_{V}

T (t)

T_{m a x}

T (t)

T^{μ ν}

T (t)

T_{m a x}

T (t)

T_{V}

T (t)

T^{μ ν}

the associated energy-momentum tensor

T (t)

t_{0}

age

T (t)

T_{m a x}

T (t)

T_{V}

T (t)

T_{V}

(highest) critical temperature

T (t)

T_{m a x}

T (t)

T^{μ ν}

T (t)

T (t_{0})

T (t)

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T (t)

T_{m a x}

T (t)

T_{V}

T (t)

T_{V}

T (t)

T_{m a x}

T (t)

T_{V}

T (t)

T_{V}

T (t)

T_{m a x}

the temperature

S_{0}

urfeld

S_{0}^{'}

S_{0}

urfeld

S_{0}^{'}

S_{0}

urfeld

S_{0}^{'}

vacuum expectation value

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

- S^{2} R_{μ}^{μ} / 12

S_{0}^{'}

- S^{2} R_{μ}^{μ} / 12

S_{0}

- S^{2} R_{μ}^{μ} / 12

S_{0}

urfeld

- S^{2} R_{μ}^{μ} / 12

S_{0}

field

- S^{2} R_{μ}^{μ} / 12

S_{0}

- S^{2} R_{μ}^{μ} / 12

S_{0}^{'}

- S^{2} R_{μ}^{μ} / 12

S_{0}

larger

- S^{2} R_{μ}^{μ} / 12

S_{0}^{'}

vacuum expectation value

- S^{2} R_{μ}^{μ} / 12

S_{0}

- S^{2} R_{μ}^{μ} / 12

S_{0}

a large rather than a small

- S^{2} R_{μ}^{μ} / 12

S_{0}

scale parameter

- S^{2} R_{μ}^{μ} / 12

S_{0}

a constant value

- S^{2} R_{μ}^{μ} / 12

S_{0}

non-zero

- S^{2} R_{μ}^{μ} / 12

S_{0}

- S^{2} R_{μ}^{μ} / 12

S_{0}

- S^{2} R_{μ}^{μ} / 12

S_{0}

background field

α > 0

α_{g}

constant

α > 0

α_{g}

constant

α > 0

α_{g}

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}^{'}

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

urfeld

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

field

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}^{'}

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

larger

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}^{'}

vacuum expectation value

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

a large rather than a small

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

scale parameter

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

a constant value

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

α_{g}

constant

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

α_{g}

constant

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

α_{g}

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

- 2 λ^{'} S_{0}^{', 2}

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

non-zero

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

α c^{2} = - 2 λ S_{0}^{2} = - 2 λ^{'} S_{0}^{', 4} / S_{0}^{2}

the parameter

S_{0}

background field

G_{e f f}

G_{F}

Fermi’s

α

matter how large

α_{g}

constant

α

matter how large

α_{g}

constant

α

matter how large

α_{g}

I_{W}

W^{μ ν}

I_{W}

W^{μ ν}

I_{W}

W^{μ ν}

__TABLE_2__

S_{0}

field

S_{0}^{'}

S_{0}

field

S_{0}^{'}

S_{0}

field

S_{0}^{'}

vacuum expectation value

ρ_{M} (t_{0})

ρ_{M} (t)

perfectly normal

ρ_{M} (t_{0})

ρ_{M} (t)

ρ_{M} (t_{0})

ρ_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

γ^{*} = - \int d r f (r) r^{2} / 2

γ_{0}

γ^{*} = - \int d r f (r) r^{2} / 2

d_{L}

- ℏ S_{0}^{2} / 12

the quantity

S_{0}^{'}

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

urfeld

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

field

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

- ℏ S_{0}^{2} / 12

the quantity

S_{0}^{'}

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

larger

- ℏ S_{0}^{2} / 12

the quantity

S_{0}^{'}

vacuum expectation value

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

a large rather than a small

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

scale parameter

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

a constant value

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

non-zero

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

- ℏ S_{0}^{2} / 12

the quantity

S_{0}

background field

{\bar{Ω}}_{M} (t = 0)

universe

{\bar{Ω}}_{Λ} (t = 0)

{\bar{Ω}}_{M} (t = 0)

universe

t_{0}

age

{\bar{Ω}}_{M} (t = 0)

universe

Ω_{M} (t = 0)

initial

{\bar{Ω}}_{M} (t = 0)

universe

Ω_{Λ} (t = 0)

initial

α

α_{g}

constant

α

α_{g}

constant

α

α_{g}

G

constant

G_{e f f}

small, negative

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{F}

Fermi’s

G

constant

G_{e f f}

G

constant

G_{e f f}

the cosmological

G

constant

G_{e f f}

a small, negative

G

constant

G_{e f f}

an appropriate

G

constant

G_{e f f}

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{k} (t)

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

future

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

S (x)

field

S_{0}^{'}

S (x)

field

S_{0}

S (x)

field

S_{0}

urfeld

S (x)

field

S_{0}

field

S (x)

field

S_{0}

S (x)

field

S_{0}^{'}

S (x)

field

S_{0}

larger

S (x)

field

S_{0}^{'}

vacuum expectation value

S (x)

field

S_{0}

S (x)

field

S_{0}

a large rather than a small

S (x)

field

S_{0}

scale parameter

S (x)

field

S_{0}

a constant value

S (x)

field

S_{0}

non-zero

S (x)

field

S_{0}

S (x)

field

S_{0}

S (x)

field

S_{0}

background field

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

t_{0}

age

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

T_{m a x} / T_{V}

such a choice

T^{4} / T_{V}^{4}

T_{m a x} / T_{V}

such a choice

T_{k i n}^{μ ν}

T_{m a x} / T_{V}

such a choice

T^{μ ν}

T_{m a x} / T_{V}

such a choice

T^{μ ν}

the associated energy-momentum tensor

T_{m a x} / T_{V}

such a choice

T^{μ ν}

T_{m a x} / T_{V}

such a choice

T_{V}^{4} / T^{4}

T_{m a x} / T_{V}

such a choice

V_{m i n}^{G L}

which

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

t_{0}

age

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

R (t) \sim e^{t}

t_{0}

age

R (t)

t_{0}

age

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T (t)

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T_{m a x} ≫ T (t_{0})

T_{V} ≫ T (t_{0})

T_{k i n}^{μ ν}

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T^{μ ν}

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T^{μ ν}

the associated energy-momentum tensor

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T_{m a x} ≫ T (t_{0})

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T^{μ ν}

T_{V} ≫ T (t_{0})

T_{m a x} ≫ T (t_{0})

T_{V} ≫ T (t_{0})

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

V_{m i n}^{G L}

which

T_{V} ≫ T (t_{0})

T_{m a x}

T_{V} ≫ T (t_{0})

T_{m a x}

the temperature

ρ_{M} (t) = σ T^{4}

T_{V}

a large

ρ_{M} (t) = σ T^{4}

T_{m a x}

ρ_{M} (t) = σ T^{4}

ρ_{M} (t_{0})

ρ_{M} (t) = σ T^{4}

T_{V}

big or small

ρ_{M} (t) = σ T^{4}

T_{V}

ρ_{M} (t) = σ T^{4}

ρ_{M} (t_{0})

ρ_{M} (t) = σ T^{4}

T_{m a x}

ρ_{M} (t) = σ T^{4}

T_{m a x}

ρ_{M} (t) = σ T^{4}

T_{k i n}^{μ ν}

ρ_{M} (t) = σ T^{4}

T_{V}

ρ_{M} (t) = σ T^{4}

T_{m a x}

ρ_{M} (t) = σ T^{4}

T^{μ ν}

ρ_{M} (t) = σ T^{4}

T_{m a x}

ρ_{M} (t) = σ T^{4}

T_{V}

ρ_{M} (t) = σ T^{4}

T^{μ ν}

the associated energy-momentum tensor

ρ_{M} (t) = σ T^{4}

t_{0}

age

ρ_{M} (t) = σ T^{4}

T_{m a x}

ρ_{M} (t) = σ T^{4}

T_{V}

ρ_{M} (t) = σ T^{4}

T_{V}

(highest) critical temperature

ρ_{M} (t) = σ T^{4}

T_{m a x}

ρ_{M} (t) = σ T^{4}

ρ_{M} (t_{0})

ρ_{M} (t) = σ T^{4}

T^{μ ν}

ρ_{M} (t) = σ T^{4}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

ρ_{M} (t) = σ T^{4}

T_{m a x}

ρ_{M} (t) = σ T^{4}

ρ_{M} (t_{0})

order

ρ_{M} (t) = σ T^{4}

T_{V}

ρ_{M} (t) = σ T^{4}

ρ_{M} (t_{0})

ρ_{M} (t) = σ T^{4}

T_{V}

ρ_{M} (t) = σ T^{4}

T_{m a x}

ρ_{M} (t) = σ T^{4}

T_{V}

ρ_{M} (t) = σ T^{4}

T_{V}

ρ_{M} (t) = σ T^{4}

T_{m a x}

the temperature

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{k} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

t_{0}

age

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

G_{F}

Fermi’s

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{Λ} (t)

- g_{00} (r) = 1 - 2 β^{*} / r + γ^{*} r

where and

γ_{0}

S_{0}

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

S_{0}^{'}

vacuum expectation value

G_{e f f}

G_{F}

Fermi’s

Ω_{M} (t = 0) + Ω_{Λ} (t = 0)

t_{0}

age

α > 0

α_{g}

constant

α > 0

α_{g}

constant

α > 0

α_{g}

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

D = 8 π G Λ / 3 c

G_{e f f}

small, negative

D = 8 π G Λ / 3 c

G_{e f f}

D = 8 π G Λ / 3 c

G_{e f f}

D = 8 π G Λ / 3 c

G_{e f f}

D = 8 π G Λ / 3 c

G_{e f f}

D = 8 π G Λ / 3 c

G_{e f f}

D = 8 π G Λ / 3 c

G_{e f f}

D = 8 π G Λ / 3 c

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

D = 8 π G Λ / 3 c

G_{e f f}

D = 8 π G Λ / 3 c

G_{e f f}

D = 8 π G Λ / 3 c

G_{e f f}

D = 8 π G Λ / 3 c

G_{F}

Fermi’s

D = 8 π G Λ / 3 c

G_{e f f}

D = 8 π G Λ / 3 c

G_{e f f}

the cosmological

D = 8 π G Λ / 3 c

G_{e f f}

a small, negative

D = 8 π G Λ / 3 c

G_{e f f}

an appropriate

D = 8 π G Λ / 3 c

G_{e f f}

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{k} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t)

t_{0}

age

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

10^{- 60}

order

10^{- 2}

order

10^{- 60}

order

10^{60}

order

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}^{'}

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

urfeld

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

field

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

L_{P L}^{- 1}

inverse Planck length

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}^{'}

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

larger

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}^{'}

vacuum expectation value

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

a large rather than a small

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

scale parameter

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

L_{P L}^{- 1}

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

a constant value

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

non-zero

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

S_{0}

background field

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = - 3 Ω_{M} (t_{0}) / 4 π S_{0}^{2} L_{P L}^{2}

Ω_{Λ} (t)

G_{e f f}

G_{F}

Fermi’s

q (t, α > 0, k < 0)

q_{0}

q (t, α > 0, k < 0)

t_{0}

age

q (t, α > 0, k < 0)

α_{g}

constant

q (t, α > 0, k < 0)

α_{g}

constant

q (t, α > 0, k < 0)

q_{0}

q (t, α > 0, k < 0)

α_{g}

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

urfeld

S_{0}^{'}

S_{0}

field

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

larger

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

a large rather than a small

S_{0}^{'}

S_{0}

scale parameter

S_{0}^{'}

S_{0}

a constant value

S_{0}^{'}

S_{0}

non-zero

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

background field

d_{L} = c H {(t_{0})}^{- 1} (z + z^{2})

L_{P L}^{- 1}

inverse Planck length

d_{L} = c H {(t_{0})}^{- 1} (z + z^{2})

L_{P L}^{- 1}

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

t_{0}

age

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{V}

a large

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{m a x}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

small, negative

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{V}

big or small

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{V}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

L_{P L}^{- 1}

inverse Planck length

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{m a x}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{m a x}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{k i n}^{μ ν}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{V}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{m a x}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T^{μ ν}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{m a x}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{V}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T^{μ ν}

the associated energy-momentum tensor

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{m a x}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{V}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{V}

(highest) critical temperature

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{m a x}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{F}

Fermi’s

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T^{μ ν}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

L_{P L}^{- 1}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{m a x}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

the cosmological

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{V}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

a small, negative

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{V}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

an appropriate

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{m a x}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{V}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{V}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

G_{e f f}

V_{m i n}^{G L} = - g {(T_{V}^{2} - T^{2})}^{2}

necessarily negative vacuum energy density

T_{m a x}

the temperature

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

T < T_{V}

T_{m a x}

T < T_{V}

T_{m a x}

T < T_{V}

T_{m a x}

T < T_{V}

T_{k i n}^{μ ν}

T < T_{V}

T_{m a x}

T < T_{V}

T^{μ ν}

T < T_{V}

T_{m a x}

T < T_{V}

T^{μ ν}

the associated energy-momentum tensor

T < T_{V}

T_{m a x}

T < T_{V}

T_{m a x}

T < T_{V}

T^{μ ν}

T < T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T < T_{V}

T_{m a x}

T < T_{V}

V_{m i n}^{G L}

which

T < T_{V}

T_{m a x}

T < T_{V}

T_{m a x}

the temperature

R^{2} (t, α = 0, k < 0)

t_{0}

age

R^{2} (t, α = 0, k < 0)

α_{g}

constant

R^{2} (t, α = 0, k < 0)

α_{g}

constant

R^{2} (t, α = 0, k < 0)

α_{g}

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

small, negative

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

D = 8 π (- G) (- Λ) / 3 c

G_{F}

Fermi’s

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

the cosmological

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

a small, negative

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

an appropriate

D = 8 π (- G) (- Λ) / 3 c

G_{e f f}

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{k} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{k} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = 1

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0}) = 1

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t)

future

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 1

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0}) = 1

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t = \infty, α > 0)

t_{0}

age

Ω_{Λ} (t = \infty, α > 0)

α_{g}

constant

Ω_{Λ} (t = \infty, α > 0)

α_{g}

constant

Ω_{Λ} (t = \infty, α > 0)

α_{g}

- 10^{60}

order

10^{- 60}

order

- 10^{60}

order

10^{- 2}

order

- 10^{60}

order

- 10^{120}

Ω_{M} (t = 0) + Ω_{Λ} (t = 0) = 1

t_{0}

age

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

T (t) ≪ T_{m a x}

all times

T_{V}

a large

T (t) ≪ T_{m a x}

all times

T_{V}

big or small

T (t) ≪ T_{m a x}

all times

T_{V}

T (t) ≪ T_{m a x}

all times

T_{k i n}^{μ ν}

T (t) ≪ T_{m a x}

all times

T (t_{0})

current temperature

T (t) ≪ T_{m a x}

all times

T_{V}

T (t) ≪ T_{m a x}

all times

T^{μ ν}

T (t) ≪ T_{m a x}

all times

T_{V}

T (t) ≪ T_{m a x}

all times

T^{μ ν}

the associated energy-momentum tensor

T (t) ≪ T_{m a x}

all times

t_{0}

age

T (t) ≪ T_{m a x}

all times

T_{V}

T (t) ≪ T_{m a x}

all times

T_{V}

(highest) critical temperature

T (t) ≪ T_{m a x}

all times

T^{μ ν}

T (t) ≪ T_{m a x}

all times

T (t_{0})

T (t) ≪ T_{m a x}

all times

T_{V}

T (t) ≪ T_{m a x}

all times

T_{V}

T (t) ≪ T_{m a x}

all times

T_{V}

T (t) ≪ T_{m a x}

all times

T_{V}

q (t) \sim 0

q (t_{0})

q (t) \sim 0

q_{0}

q (t) \sim 0

q (t_{0})

q (t) \sim 0

q (t_{0})

q (t) \sim 0

t_{0}

age

q (t) \sim 0

q_{0}

q (t) \sim 0

q (t_{0})

q (t) \sim 0

q (t_{0})

q (t) \sim 0

q (t_{0})

G

effective

G_{e f f}

small, negative

G

effective

G_{e f f}

G

effective

G_{e f f}

G

effective

G_{e f f}

G

effective

G_{e f f}

G

effective

G_{e f f}

G

effective

G_{e f f}

G

effective

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

effective

G_{e f f}

G

effective

G_{e f f}

G

effective

G_{e f f}

G

effective

G_{F}

Fermi’s

G

effective

G_{e f f}

G

effective

G_{e f f}

the cosmological

G

effective

G_{e f f}

a small, negative

G

effective

G_{e f f}

an appropriate

G

effective

G_{e f f}

G_{e f f}

G_{F}

Fermi’s

α > 0

α_{g}

constant

α > 0

α_{g}

constant

α > 0

α_{g}

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

t_{0}

age

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

s e c h^{2} (α^{1 / 2} c t_{0})

α_{g}

constant

s e c h^{2} (α^{1 / 2} c t_{0})

α_{g}

constant

s e c h^{2} (α^{1 / 2} c t_{0})

α_{g}

T_{m a x}

T_{V}

a large

T_{m a x}

T_{V}

big or small

T_{m a x}

T_{V}

T_{m a x}

T_{k i n}^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T_{V}

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{k} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

negative

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

control

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

future

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}^{'}

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

urfeld

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

field

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}^{'}

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

larger

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}^{'}

vacuum expectation value

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

a large rather than a small

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

scale parameter

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

G_{F}

Fermi’s

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

a constant value

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

non-zero

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

G_{e f f} = - 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

background field

G_{e f f}

G_{F}

Fermi’s

T_{m a x}

T_{V}

a large

T_{m a x}

T_{V}

big or small

T_{m a x}

T_{V}

T_{m a x}

T_{k i n}^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T_{V}

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{V} ≃ 10^{16} {}^{\circ}K

T_{m a x}

T_{V} ≃ 10^{16} {}^{\circ}K

10^{- 60}

order

T_{V} ≃ 10^{16} {}^{\circ}K

T_{m a x}

T_{V} ≃ 10^{16} {}^{\circ}K

T_{m a x}

T_{V} ≃ 10^{16} {}^{\circ}K

T_{k i n}^{μ ν}

T_{V} ≃ 10^{16} {}^{\circ}K

T_{m a x}

T_{V} ≃ 10^{16} {}^{\circ}K

T^{μ ν}

T_{V} ≃ 10^{16} {}^{\circ}K

T_{m a x}

T_{V} ≃ 10^{16} {}^{\circ}K

T^{μ ν}

the associated energy-momentum tensor

T_{V} ≃ 10^{16} {}^{\circ}K

T_{m a x}

T_{V} ≃ 10^{16} {}^{\circ}K

T_{m a x}

T_{V} ≃ 10^{16} {}^{\circ}K

T^{μ ν}

T_{V} ≃ 10^{16} {}^{\circ}K

10^{- 2}

order

T_{V} ≃ 10^{16} {}^{\circ}K

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V} ≃ 10^{16} {}^{\circ}K

T_{m a x}

T_{V} ≃ 10^{16} {}^{\circ}K

V_{m i n}^{G L}

which

T_{V} ≃ 10^{16} {}^{\circ}K

10^{60}

order

T_{V} ≃ 10^{16} {}^{\circ}K

T_{m a x}

T_{V} ≃ 10^{16} {}^{\circ}K

T_{m a x}

the temperature

t a n h^{2} (α^{1 / 2} c t_{0})

t a n h (α^{1 / 2} c t_{0})

t a n h^{2} (α^{1 / 2} c t_{0})

α_{g}

constant

t a n h^{2} (α^{1 / 2} c t_{0})

α_{g}

constant

t a n h^{2} (α^{1 / 2} c t_{0})

α_{g}

T^{4} / T_{V}^{4}

T_{V}

a large

T^{4} / T_{V}^{4}

T_{m a x}

T^{4} / T_{V}^{4}

T_{V}

big or small

T^{4} / T_{V}^{4}

T_{V}

T^{4} / T_{V}^{4}

T_{m a x} / T_{V}

such a choice

T^{4} / T_{V}^{4}

T_{m a x}

T^{4} / T_{V}^{4}

T_{m a x}

T^{4} / T_{V}^{4}

T_{k i n}^{μ ν}

T^{4} / T_{V}^{4}

T_{V}

T^{4} / T_{V}^{4}

T_{m a x}

T^{4} / T_{V}^{4}

T^{μ ν}

T^{4} / T_{V}^{4}

T_{m a x}

T^{4} / T_{V}^{4}

T_{V}

T^{4} / T_{V}^{4}

T^{μ ν}

the associated energy-momentum tensor

T^{4} / T_{V}^{4}

T_{m a x}

T^{4} / T_{V}^{4}

T_{V}

T^{4} / T_{V}^{4}

T_{V}

(highest) critical temperature

T^{4} / T_{V}^{4}

T_{m a x}

T^{4} / T_{V}^{4}

T^{μ ν}

T^{4} / T_{V}^{4}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T^{4} / T_{V}^{4}

T_{m a x}

T^{4} / T_{V}^{4}

T_{V}^{4} / T^{4}

T^{4} / T_{V}^{4}

T_{V}

T^{4} / T_{V}^{4}

V_{m i n}^{G L}

which

T^{4} / T_{V}^{4}

T_{V}

T^{4} / T_{V}^{4}

T_{m a x}

T^{4} / T_{V}^{4}

T_{V}

T^{4} / T_{V}^{4}

T_{V}

T^{4} / T_{V}^{4}

T_{m a x}

the temperature

\dot{R} (t) / R (t) = α^{1 / 2} c

R (t)

\dot{R} (t) / R (t) = α^{1 / 2} c

R (t)

\dot{R} (t) / R (t) = α^{1 / 2} c

t_{0}

age

\dot{R} (t) / R (t) = α^{1 / 2} c

α c^{2}

\dot{R} (t) / R (t) = α^{1 / 2} c

α_{g}

constant

\dot{R} (t) / R (t) = α^{1 / 2} c

α_{g}

constant

\dot{R} (t) / R (t) = α^{1 / 2} c

α_{g}

\dot{R} (t) / R (t) = α^{1 / 2} c

R (t)

q (t_{0})

q_{0}

q (t_{0})

q (t)

conformal cosmology

q (t_{0})

q (t)

q (t_{0})

q_{0}

α > 0, k = 0

α_{g}

constant

α > 0, k = 0

α_{g}

constant

α > 0, k = 0

α_{g}

α > 0

α_{g}

constant

α > 0

α_{g}

constant

α > 0

α_{g}

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{k} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{k} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

negative

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

control

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

future

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

q (t_{0})

q_{0}

q (t_{0})

q (t)

conformal cosmology

q (t_{0})

q (t)

q (t_{0})

q_{0}

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

future

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

T_{m a x} ≫ T (t_{0})

T_{V}

a large

T_{m a x} ≫ T (t_{0})

T_{V} ≫ T (t_{0})

T_{m a x} ≫ T (t_{0})

T_{V}

big or small

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T (t)

T_{m a x} ≫ T (t_{0})

T_{V} ≫ T (t_{0})

T_{m a x} ≫ T (t_{0})

T_{k i n}^{μ ν}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T^{μ ν}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T^{μ ν}

the associated energy-momentum tensor

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T_{V}

(highest) critical temperature

T_{m a x} ≫ T (t_{0})

T^{μ ν}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T_{V}

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{k} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t)

t_{0}

age

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

T_{k i n}^{μ ν}

T_{V}

a large

T_{k i n}^{μ ν}

T_{m a x}

T_{k i n}^{μ ν}

T_{V}

big or small

T_{k i n}^{μ ν}

T_{V}

T_{k i n}^{μ ν}

T_{m a x}

T_{k i n}^{μ ν}

T_{m a x}

T_{k i n}^{μ ν}

T_{V}

T_{k i n}^{μ ν}

T_{m a x}

T_{k i n}^{μ ν}

T^{μ ν}

T_{k i n}^{μ ν}

T_{m a x}

T_{k i n}^{μ ν}

T_{V}

T_{k i n}^{μ ν}

T^{μ ν}

the associated energy-momentum tensor

T_{k i n}^{μ ν}

T_{m a x}

T_{k i n}^{μ ν}

T_{V}

T_{k i n}^{μ ν}

T_{V}

(highest) critical temperature

T_{k i n}^{μ ν}

T_{m a x}

T_{k i n}^{μ ν}

T^{μ ν}

T_{k i n}^{μ ν}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{k i n}^{μ ν}

T_{m a x}

T_{k i n}^{μ ν}

T_{V}

T_{k i n}^{μ ν}

T_{V}

T_{k i n}^{μ ν}

T_{m a x}

T_{k i n}^{μ ν}

T_{V}

T_{k i n}^{μ ν}

T_{V}

T_{k i n}^{μ ν}

T_{m a x}

the temperature

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t, α > 0, k > 0)

the positive spatial 3-curvature

t_{0}

age

Ω_{Λ} (t, α > 0, k > 0)

the positive spatial 3-curvature

α_{g}

constant

Ω_{Λ} (t, α > 0, k > 0)

the positive spatial 3-curvature

α_{g}

constant

Ω_{Λ} (t, α > 0, k > 0)

the positive spatial 3-curvature

α_{g}

α > 0

α_{g}

constant

α > 0

α_{g}

constant

α > 0

α_{g}

α > 0

α_{g}

constant

α > 0

α_{g}

constant

α > 0

α_{g}

Λ = ℏ λ S_{0}^{4}

S_{0}^{'}

Λ = ℏ λ S_{0}^{4}

S_{0}

Λ = ℏ λ S_{0}^{4}

S_{0}

urfeld

Λ = ℏ λ S_{0}^{4}

S_{0}

field

Λ = ℏ λ S_{0}^{4}

S_{0}

Λ = ℏ λ S_{0}^{4}

S_{0}^{'}

Λ = ℏ λ S_{0}^{4}

S_{0}

larger

Λ = ℏ λ S_{0}^{4}

S_{0}^{'}

vacuum expectation value

Λ = ℏ λ S_{0}^{4}

S_{0}

Λ = ℏ λ S_{0}^{4}

S_{0}

a large rather than a small

Λ = ℏ λ S_{0}^{4}

S_{0}

scale parameter

Λ = ℏ λ S_{0}^{4}

S_{0}

a constant value

Λ = ℏ λ S_{0}^{4}

S_{0}

non-zero

Λ = ℏ λ S_{0}^{4}

S_{0}

Λ = ℏ λ S_{0}^{4}

S_{0}

Λ = ℏ λ S_{0}^{4}

S_{0}

background field

{\bar{Ω}}_{Λ} (t = 0)

{\bar{Ω}}_{M} (t = 0)

universe

{\bar{Ω}}_{Λ} (t = 0)

t_{0}

age

{\bar{Ω}}_{Λ} (t = 0)

{\bar{Ω}}_{M} (t = 0)

{\bar{Ω}}_{Λ} (t = 0)

Ω_{M} (t = 0)

initial

{\bar{Ω}}_{Λ} (t = 0)

Ω_{Λ} (t = 0)

initial

α

the parameter

α_{g}

constant

α

the parameter

α_{g}

constant

α

the parameter

α_{g}

α > 0

α_{g}

constant

α > 0

α_{g}

constant

α > 0

α_{g}

q (t) \sim - \infty

q (t_{0})

q (t) \sim - \infty

q_{0}

q (t) \sim - \infty

q (t_{0})

q (t) \sim - \infty

q (t_{0})

q (t) \sim - \infty

t_{0}

age

q (t) \sim - \infty

q_{0}

q (t) \sim - \infty

q (t_{0})

q (t) \sim - \infty

q (t_{0})

q (t) \sim - \infty

q (t_{0})

α > 0

α_{g}

constant

α > 0

α_{g}

constant

α > 0

α_{g}

T (t_{0})

current temperature

T_{V}

a large

T (t_{0})

current temperature

T_{m a x}

T (t_{0})

current temperature

T_{V}

big or small

T (t_{0})

current temperature

T_{V}

T (t_{0})

current temperature

T (t)

T (t_{0})

current temperature

T_{m a x}

T (t_{0})

current temperature

T_{m a x}

T (t_{0})

current temperature

T_{k i n}^{μ ν}

T (t_{0})

current temperature

T_{V}

T (t_{0})

current temperature

T_{m a x}

T (t_{0})

current temperature

T^{μ ν}

T (t_{0})

current temperature

T_{m a x}

T (t_{0})

current temperature

T_{V}

T (t_{0})

current temperature

T^{μ ν}

the associated energy-momentum tensor

T (t_{0})

current temperature

T_{m a x}

T (t_{0})

current temperature

T_{V}

T (t_{0})

current temperature

T_{V}

(highest) critical temperature

T (t_{0})

current temperature

T_{m a x}

T (t_{0})

current temperature

T^{μ ν}

T (t_{0})

current temperature

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T (t_{0})

current temperature

T_{m a x}

T (t_{0})

current temperature

T_{V}

T (t_{0})

current temperature

T_{V}

T (t_{0})

current temperature

T_{m a x}

T (t_{0})

current temperature

T_{V}

T (t_{0})

current temperature

T_{V}

T (t_{0})

current temperature

T_{m a x}

the temperature

G_{e f f}

G_{F}

Fermi’s

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

t a n h (α^{1 / 2} c t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

α_{g}

constant

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

α_{g}

constant

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

α_{g}

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0}) = t a n h^{2} (α^{1 / 2} c t_{0})

Ω_{Λ} (t)

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{k i n}^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

T_{V}

V_{m i n}^{G L}

which

T_{V}

T_{m a x}

T_{V}

T_{m a x}

the temperature

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t)

t_{0}

age

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G_{F}

Fermi’s

S (x) = 0

S_{0}^{'}

S (x) = 0

S_{0}

S (x) = 0

S_{0}

urfeld

S (x) = 0

S_{0}

field

S (x) = 0

S_{0}

S (x) = 0

S_{0}^{'}

S (x) = 0

S_{0}

larger

S (x) = 0

S_{0}^{'}

vacuum expectation value

S (x) = 0

S_{0}

S (x) = 0

S_{0}

a large rather than a small

S (x) = 0

S_{0}

scale parameter

S (x) = 0

S_{0}

a constant value

S (x) = 0

S_{0}

non-zero

S (x) = 0

S_{0}

S (x) = 0

S_{0}

S (x) = 0

S_{0}

background field

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

t_{0}

age

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

t = 0

t_{0}

age

t = \int d τ / R (τ)

t_{0}

age

t = \int d τ / R (τ)

d_{L}

c | Λ | = σ T_{V}^{4}

T_{V}

a large

c | Λ | = σ T_{V}^{4}

T_{m a x}

c | Λ | = σ T_{V}^{4}

T_{V}

big or small

c | Λ | = σ T_{V}^{4}

T_{V}

c | Λ | = σ T_{V}^{4}

T_{m a x}

c | Λ | = σ T_{V}^{4}

T_{m a x}

c | Λ | = σ T_{V}^{4}

T_{k i n}^{μ ν}

c | Λ | = σ T_{V}^{4}

T_{V}

c | Λ | = σ T_{V}^{4}

T_{m a x}

c | Λ | = σ T_{V}^{4}

T^{μ ν}

c | Λ | = σ T_{V}^{4}

T_{m a x}

c | Λ | = σ T_{V}^{4}

T_{V}

c | Λ | = σ T_{V}^{4}

T^{μ ν}

the associated energy-momentum tensor

c | Λ | = σ T_{V}^{4}

T_{m a x}

c | Λ | = σ T_{V}^{4}

T_{V}

c | Λ | = σ T_{V}^{4}

T_{V}

(highest) critical temperature

c | Λ | = σ T_{V}^{4}

T_{m a x}

c | Λ | = σ T_{V}^{4}

T^{μ ν}

c | Λ | = σ T_{V}^{4}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

c | Λ | = σ T_{V}^{4}

T_{m a x}

c | Λ | = σ T_{V}^{4}

T_{V}

c | Λ | = σ T_{V}^{4}

V_{m i n}^{G L}

which

c | Λ | = σ T_{V}^{4}

T_{V}

c | Λ | = σ T_{V}^{4}

T_{m a x}

c | Λ | = σ T_{V}^{4}

T_{V}

c | Λ | = σ T_{V}^{4}

T_{V}

c | Λ | = σ T_{V}^{4}

T_{m a x}

the temperature

\dot{R} (t = 0)

t_{0}

age

α = 8 π G_{e f f} Λ / 3 c^{3}

G_{F}

Fermi’s

α = 8 π G_{e f f} Λ / 3 c^{3}

α_{g}

constant

α = 8 π G_{e f f} Λ / 3 c^{3}

α_{g}

constant

α = 8 π G_{e f f} Λ / 3 c^{3}

α_{g}

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{k} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

t_{0}

age

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t)

future

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

α_{g}

constant

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

α_{g}

constant

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

α_{g}

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t) = α c^{2} R^{2} (t) / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

S (x)

S_{0}^{'}

S (x)

S_{0}

S (x)

S_{0}

urfeld

S (x)

S_{0}

field

S (x)

S_{0}

S (x)

S_{0}^{'}

S (x)

S_{0}

larger

S (x)

S_{0}^{'}

vacuum expectation value

S (x)

S_{0}

S (x)

S_{0}

a large rather than a small

S (x)

S_{0}

scale parameter

S (x)

S_{0}

a constant value

S (x)

S_{0}

non-zero

S (x)

S_{0}

S (x)

S_{0}

S (x)

S_{0}

background field

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

t_{0}

age

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

t_{0}

age

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

G_{F}

Fermi’s

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

ρ_{M} (t) = B / R^{3}

ρ_{M} (t_{0})

ρ_{M} (t) = B / R^{3}

ρ_{M} (t_{0})

ρ_{M} (t) = B / R^{3}

t_{0}

age

ρ_{M} (t) = B / R^{3}

ρ_{M} (t_{0})

ρ_{M} (t) = B / R^{3}

ρ_{M} (t_{0})

order

ρ_{M} (t) = B / R^{3}

ρ_{M} (t_{0})

T_{m a x}

T_{V}

a large

T_{m a x}

T_{V}

big or small

T_{m a x}

T_{V}

T_{m a x}

T_{k i n}^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T_{V}

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{k} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{k} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

t_{0}

age

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t)

future

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

S (x)

field

S_{0}^{'}

S (x)

field

S_{0}

S (x)

field

S_{0}

urfeld

S (x)

field

S_{0}

field

S (x)

field

S_{0}

S (x)

field

S_{0}^{'}

S (x)

field

S_{0}

larger

S (x)

field

S_{0}^{'}

vacuum expectation value

S (x)

field

S_{0}

S (x)

field

S_{0}

a large rather than a small

S (x)

field

S_{0}

scale parameter

S (x)

field

S_{0}

a constant value

S (x)

field

S_{0}

non-zero

S (x)

field

S_{0}

S (x)

field

S_{0}

S (x)

field

S_{0}

background field

R (t)

t_{0}

age

T^{μ ν}

T_{V}

a large

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{V}

big or small

T^{μ ν}

T_{V}

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{k i n}^{μ ν}

T^{μ ν}

T_{V}

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{V}

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{V}

T^{μ ν}

T_{V}

(highest) critical temperature

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{V}

T^{μ ν}

T_{V}

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{V}

T^{μ ν}

T_{V}

T^{μ ν}

T_{m a x}

the temperature

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

q (t_{0}) = - 1

the deceleration parameter

q_{0}

q (t_{0}) = - 1

the deceleration parameter

q (t)

conformal cosmology

q (t_{0}) = - 1

the deceleration parameter

q (t)

q (t_{0}) = - 1

the deceleration parameter

q_{0}

T_{m a x}

T_{V}

a large

T_{m a x}

T_{V}

big or small

T_{m a x}

T_{V}

T_{m a x}

T_{k i n}^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T_{V}

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{k i n}^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

T_{V}

V_{m i n}^{G L}

which

T_{V}

T_{m a x}

T_{V}

T_{m a x}

the temperature

T^{μ ν}

the associated energy-momentum tensor

T_{V}

a large

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

big or small

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{k i n}^{μ ν}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

(highest) critical temperature

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

the temperature

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{k} (t)

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{k} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

t_{0}

age

Ω_{Λ} (t)

control

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t)

future

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t)

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

control

Ω_{M} (t)

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

ρ_{M} (t) = A / R^{n} (t)

ρ_{M} (t_{0})

ρ_{M} (t) = A / R^{n} (t)

ρ_{M} (t_{0})

ρ_{M} (t) = A / R^{n} (t)

t_{0}

age

ρ_{M} (t) = A / R^{n} (t)

ρ_{M} (t_{0})

ρ_{M} (t) = A / R^{n} (t)

ρ_{M} (t_{0})

order

ρ_{M} (t) = A / R^{n} (t)

ρ_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t)

t_{0}

age

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{k} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{k} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

negative

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

control

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

future

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{k} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{k} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

the current era

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

negative

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

control

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

the current era

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

the same order of magnitude

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

future

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

the standard model

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

the current era

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{k} (t_{0})

orders

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t_{0})

era

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

0 \leq Ω_{Λ} (t) \leq 1

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{k} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

the current era

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

negative

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

control

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

t_{0}

age

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t)

future

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

the current era

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{M} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{k} (t_{0})

orders

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t) = - k c^{2} / {\dot{R}}^{2} (t)

Ω_{Λ} (t)

S_{0}

larger

S_{0}^{'}

S_{0}

larger

S_{0}^{'}

S_{0}

larger

S_{0}^{'}

vacuum expectation value

G_{e f f}

G_{F}

Fermi’s

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{k} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{k} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t)

future

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0}) \approx 0.7

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) \approx 0.7

Ω_{Λ} (t)

t a n h (α^{1 / 2} c t_{0})

t a n h^{2} (α^{1 / 2} c t_{0})

t a n h (α^{1 / 2} c t_{0})

α_{g}

constant

t a n h (α^{1 / 2} c t_{0})

α_{g}

constant

t a n h (α^{1 / 2} c t_{0})

α_{g}

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0}) = 8 π G ρ_{M} (t_{0}) / 3 c^{2} H^{2} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

small, negative

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{k} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{k} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{M} (t) = 8 π G_{e f f} ρ_{M} (t) / 3 c^{2} H^{2} (t)

effective

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

control

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

t_{0}

age

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{F}

Fermi’s

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

the cosmological

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

a small, negative

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{M} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

an appropriate

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

G_{e f f}

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t) = 8 π G ρ_{M} (t) / 3 c^{2} H^{2} (t)

Ω_{Λ} (t)

T_{m a x}

T_{V}

a large

T_{m a x}

T_{V}

big or small

T_{m a x}

T_{V}

T_{m a x}

T_{k i n}^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T_{V}

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

α

α_{g}

constant

α

α_{g}

constant

α

α_{g}

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

q (t)

conformal cosmology

q (t_{0})

q (t)

conformal cosmology

q_{0}

q (t)

conformal cosmology

q (t_{0})

q (t)

conformal cosmology

q (t_{0})

q (t)

conformal cosmology

t_{0}

age

q (t)

conformal cosmology

q_{0}

q (t)

conformal cosmology

q (t_{0})

q (t)

conformal cosmology

q (t_{0})

q (t)

conformal cosmology

q (t_{0})

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{k i n}^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

T_{V}

V_{m i n}^{G L}

which

T_{V}

T_{m a x}

T_{V}

T_{m a x}

the temperature

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{k} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0}) = 1

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

negative

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

control

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

future

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0}) = 1

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

T_{V}

(highest) critical temperature

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

T_{V}

(highest) critical temperature

T_{k i n}^{μ ν}

T_{V}

(highest) critical temperature

T_{m a x}

T_{V}

(highest) critical temperature

T^{μ ν}

T_{V}

(highest) critical temperature

T_{m a x}

T_{V}

(highest) critical temperature

T^{μ ν}

the associated energy-momentum tensor

T_{V}

(highest) critical temperature

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

T_{V}

(highest) critical temperature

T^{μ ν}

T_{V}

(highest) critical temperature

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

(highest) critical temperature

T_{m a x}

T_{V}

(highest) critical temperature

V_{m i n}^{G L}

which

T_{V}

(highest) critical temperature

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

the temperature

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{k} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0}) = 1

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

negative

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

control

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

future

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0}) = 1

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

small, negative

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{k} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

t_{0}

age

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t)

future

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{F}

Fermi’s

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

the cosmological

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

a small, negative

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

an appropriate

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

G_{e f f}

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

d_{L} = c H {(t_{0})}^{- 1} (z + z^{2} / 2)

L_{P L}^{- 1}

inverse Planck length

d_{L} = c H {(t_{0})}^{- 1} (z + z^{2} / 2)

L_{P L}^{- 1}

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

T_{m a x} ≫ T (t_{0})

T_{V}

a large

T_{m a x} ≫ T (t_{0})

T_{V} ≫ T (t_{0})

T_{m a x} ≫ T (t_{0})

T_{V}

big or small

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T (t)

T_{m a x} ≫ T (t_{0})

T_{V} ≫ T (t_{0})

T_{m a x} ≫ T (t_{0})

T_{k i n}^{μ ν}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T^{μ ν}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T^{μ ν}

the associated energy-momentum tensor

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T_{V}

(highest) critical temperature

T_{m a x} ≫ T (t_{0})

T^{μ ν}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T_{V}

S_{0}^{'}

vacuum expectation value

S_{0}

S_{0}^{'}

vacuum expectation value

S_{0}

urfeld

S_{0}^{'}

vacuum expectation value

S_{0}

field

S_{0}^{'}

vacuum expectation value

S_{0}

S_{0}^{'}

vacuum expectation value

S_{0}

larger

S_{0}^{'}

vacuum expectation value

S_{0}

S_{0}^{'}

vacuum expectation value

S_{0}

a large rather than a small

S_{0}^{'}

vacuum expectation value

S_{0}

scale parameter

S_{0}^{'}

vacuum expectation value

S_{0}

a constant value

S_{0}^{'}

vacuum expectation value

S_{0}

non-zero

S_{0}^{'}

vacuum expectation value

S_{0}

S_{0}^{'}

vacuum expectation value

S_{0}

S_{0}^{'}

vacuum expectation value

S_{0}

background field

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

- g_{00} (r) = 1 - 2 β^{*} / r + γ^{*} r

γ_{0}

G

constant

G_{e f f}

small, negative

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{e f f}

G

constant

G_{F}

Fermi’s

G

constant

G_{e f f}

G

constant

G_{e f f}

the cosmological

G

constant

G_{e f f}

a small, negative

G

constant

G_{e f f}

an appropriate

G

constant

G_{e f f}

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

α = - 2 λ S_{0}^{2}

parameters

S_{0}^{'}

α = - 2 λ S_{0}^{2}

parameters

S_{0}

α = - 2 λ S_{0}^{2}

parameters

S_{0}

urfeld

α = - 2 λ S_{0}^{2}

parameters

S_{0}

field

α = - 2 λ S_{0}^{2}

parameters

S_{0}

α = - 2 λ S_{0}^{2}

parameters

S_{0}^{'}

α = - 2 λ S_{0}^{2}

parameters

S_{0}

larger

α = - 2 λ S_{0}^{2}

parameters

S_{0}^{'}

vacuum expectation value

α = - 2 λ S_{0}^{2}

parameters

S_{0}

α = - 2 λ S_{0}^{2}

parameters

S_{0}

a large rather than a small

α = - 2 λ S_{0}^{2}

parameters

S_{0}

scale parameter

α = - 2 λ S_{0}^{2}

parameters

S_{0}

a constant value

α = - 2 λ S_{0}^{2}

parameters

α_{g}

constant

α = - 2 λ S_{0}^{2}

parameters

α_{g}

constant

α = - 2 λ S_{0}^{2}

parameters

α_{g}

α = - 2 λ S_{0}^{2}

parameters

- 2 λ^{'} S_{0}^{', 2}

α = - 2 λ S_{0}^{2}

parameters

S_{0}

non-zero

α = - 2 λ S_{0}^{2}

parameters

S_{0}

α = - 2 λ S_{0}^{2}

parameters

S_{0}

α = - 2 λ S_{0}^{2}

parameters

S_{0}

background field

q (t)

q (t_{0})

q (t)

q_{0}

q (t)

q (t_{0})

q (t)

q (t_{0})

q (t)

t_{0}

age

q (t)

q_{0}

q (t)

q (t_{0})

q (t)

q (t_{0})

q (t)

q (t_{0})

α

the parameter

α_{g}

constant

α

the parameter

α_{g}

constant

α

the parameter

α_{g}

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

ρ_{M} (t) > 0

ρ_{M} (t_{0})

ρ_{M} (t) > 0

ρ_{M} (t_{0})

ρ_{M} (t) > 0

t_{0}

age

ρ_{M} (t) > 0

ρ_{M} (t_{0})

ρ_{M} (t) > 0

ρ_{M} (t_{0})

order

ρ_{M} (t) > 0

ρ_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

d s^{2} = Ω (τ, ρ) [c^{2} d τ^{2} - R^{2} (τ) (d ρ^{2} + ρ^{2} d Ω) / {(1 - ρ^{2} γ_{0}^{2} / 16)}^{2}]

γ_{0}

d s^{2} = Ω (τ, ρ) [c^{2} d τ^{2} - R^{2} (τ) (d ρ^{2} + ρ^{2} d Ω) / {(1 - ρ^{2} γ_{0}^{2} / 16)}^{2}]

d_{L}

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{k} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{k} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

the current era

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

negative

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

control

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

the current era

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

the same order of magnitude

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

future

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

the standard model

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

the current era

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{M} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{k} (t_{0})

orders

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

{\bar{Ω}}_{M} (t_{0})

era

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

0 \leq Ω_{Λ} (t) \leq 1

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t_{0})

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t, α = 0, k < 0)

t_{0}

age

Ω_{Λ} (t, α = 0, k < 0)

α_{g}

constant

Ω_{Λ} (t, α = 0, k < 0)

α_{g}

constant

Ω_{Λ} (t, α = 0, k < 0)

α_{g}

α < 0

α_{g}

constant

α < 0

α_{g}

constant

α < 0

α_{g}

G_{e f f}

G_{F}

Fermi’s

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t)

t_{0}

age

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

α

α_{g}

constant

α

α_{g}

constant

α

α_{g}

T_{k i n}^{μ ν} = 0

T_{V}

a large

T_{k i n}^{μ ν} = 0

T_{m a x}

T_{k i n}^{μ ν} = 0

T_{V}

big or small

T_{k i n}^{μ ν} = 0

T_{V}

T_{k i n}^{μ ν} = 0

T_{m a x}

T_{k i n}^{μ ν} = 0

T_{m a x}

T_{k i n}^{μ ν} = 0

T_{V}

T_{k i n}^{μ ν} = 0

T_{m a x}

T_{k i n}^{μ ν} = 0

T^{μ ν}

T_{k i n}^{μ ν} = 0

T_{m a x}

T_{k i n}^{μ ν} = 0

T_{V}

T_{k i n}^{μ ν} = 0

T^{μ ν}

the associated energy-momentum tensor

T_{k i n}^{μ ν} = 0

T_{m a x}

T_{k i n}^{μ ν} = 0

T_{V}

T_{k i n}^{μ ν} = 0

T_{V}

(highest) critical temperature

T_{k i n}^{μ ν} = 0

T_{m a x}

T_{k i n}^{μ ν} = 0

T^{μ ν}

T_{k i n}^{μ ν} = 0

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{k i n}^{μ ν} = 0

T_{m a x}

T_{k i n}^{μ ν} = 0

T_{V}

T_{k i n}^{μ ν} = 0

T_{V}

T_{k i n}^{μ ν} = 0

T^{μ ν} = 0

motion

T_{k i n}^{μ ν} = 0

T_{m a x}

T_{k i n}^{μ ν} = 0

T_{V}

T_{k i n}^{μ ν} = 0

T_{V}

T_{k i n}^{μ ν} = 0

T_{m a x}

the temperature

α c^{2}

α_{g}

constant

α c^{2}

α_{g}

constant

α c^{2}

α_{g}

T_{m a x}

T_{V}

a large

T_{m a x}

T_{V}

big or small

T_{m a x}

T_{V}

T_{m a x}

T_{k i n}^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T_{V}

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

S_{0}

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

S_{0}^{'}

vacuum expectation value

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

α \geq 0

α_{g}

constant

α \geq 0

α_{g}

constant

α \geq 0

α_{g}

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

t_{0}

age

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t) = 8 π G Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

G_{F}

Fermi’s

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) = 8 π G_{e f f} Λ / 3 c H^{2} (t)

Ω_{Λ} (t)

c^{3} / 16 π G

G_{e f f}

small, negative

c^{3} / 16 π G

G_{e f f}

c^{3} / 16 π G

G_{e f f}

c^{3} / 16 π G

G_{e f f}

c^{3} / 16 π G

G_{e f f}

c^{3} / 16 π G

G_{e f f}

c^{3} / 16 π G

G_{e f f}

c^{3} / 16 π G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

c^{3} / 16 π G

G_{e f f}

c^{3} / 16 π G

G_{e f f}

c^{3} / 16 π G

G_{e f f}

c^{3} / 16 π G

G_{F}

Fermi’s

c^{3} / 16 π G

G_{e f f}

c^{3} / 16 π G

G_{e f f}

the cosmological

c^{3} / 16 π G

G_{e f f}

a small, negative

c^{3} / 16 π G

G_{e f f}

an appropriate

c^{3} / 16 π G

G_{e f f}

G_{e f f}

G_{F}

Fermi’s

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{k} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t) = O (10^{- 60})

t_{0}

age

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

10^{- 2}

order

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

10^{60}

order

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{M} (t) = O (10^{- 60})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t) = O (10^{- 60})

Ω_{Λ} (t)

α

α_{g}

constant

α

α_{g}

constant

α

α_{g}

R (t) \sim e^{t}

t_{0}

age

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{k} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

negative

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

control

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

future

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

- q (t_{0}) H^{2} (t_{0}) = α c^{2}

q_{0}

- q (t_{0}) H^{2} (t_{0}) = α c^{2}

α_{g}

constant

- q (t_{0}) H^{2} (t_{0}) = α c^{2}

α_{g}

constant

- q (t_{0}) H^{2} (t_{0}) = α c^{2}

q_{0}

- q (t_{0}) H^{2} (t_{0}) = α c^{2}

α_{g}

- q (t_{0}) H^{2} (t_{0}) = α c^{2}

- q (t) H^{2} (t)

Ω_{Λ} (t, α > 0)

the faster

t_{0}

age

Ω_{Λ} (t, α > 0)

the faster

α_{g}

constant

Ω_{Λ} (t, α > 0)

the faster

α_{g}

constant

Ω_{Λ} (t, α > 0)

the faster

α_{g}

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{k} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{k} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

future

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

α

α_{g}

constant

α

α_{g}

constant

α

α_{g}

α = 0

α_{g}

constant

α = 0

α_{g}

constant

α = 0

α_{g}

H^{2} (t_{0}) = - α c^{2} / q (t_{0})

q_{0}

H^{2} (t_{0}) = - α c^{2} / q (t_{0})

α_{g}

constant

H^{2} (t_{0}) = - α c^{2} / q (t_{0})

α_{g}

constant

H^{2} (t_{0}) = - α c^{2} / q (t_{0})

q_{0}

H^{2} (t_{0}) = - α c^{2} / q (t_{0})

α_{g}

ρ_{M} (t_{0})

ρ_{M} (t)

perfectly normal

ρ_{M} (t_{0})

ρ_{M} (t)

ρ_{M} (t_{0})

ρ_{M} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{k} (t)

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{k} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

negative

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t)

control

Ω_{M} (t)

future

t_{0}

age

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{k} (t_{0})

orders

Ω_{M} (t)

future

Ω_{Λ} (t)

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

future

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t)

t_{0}

age

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

S_{0}

a large rather than a small

S_{0}^{'}

S_{0}

a large rather than a small

S_{0}^{'}

S_{0}

a large rather than a small

S_{0}^{'}

vacuum expectation value

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{V}

a large

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{m a x}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{V}

big or small

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{V}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{m a x}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{m a x}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{k i n}^{μ ν}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{V}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{m a x}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T^{μ ν}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{m a x}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{V}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T^{μ ν}

the associated energy-momentum tensor

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{m a x}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{V}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{V}

(highest) critical temperature

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{m a x}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T^{μ ν}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{m a x}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{V}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

V_{m i n}^{G L}

which

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{V}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{m a x}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{V}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{V}

T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4}

the quantity

T_{m a x}

the temperature

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{V}

a large

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{m a x}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{V}

big or small

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{V}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{m a x}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{m a x}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{k i n}^{μ ν}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{V}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{m a x}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T^{μ ν}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{m a x}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{V}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T^{μ ν}

the associated energy-momentum tensor

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

t a n h (α^{1 / 2} c t_{0})

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{m a x}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{V}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{V}

(highest) critical temperature

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{m a x}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T^{μ ν}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

α_{g}

constant

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

α_{g}

constant

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{m a x}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

α_{g}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{V}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

V_{m i n}^{G L}

which

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{V}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{m a x}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{V}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{V}

- t a n h^{2} (α^{1 / 2} c t_{0}) = - {(1 + T^{2} (t_{0}) T_{m a x}^{2} / T_{V}^{4})}^{- 1}

T_{m a x}

the temperature

ρ_{M} (t)

ρ_{M} (t_{0})

ρ_{M} (t)

ρ_{M} (t_{0})

ρ_{M} (t)

t_{0}

age

ρ_{M} (t)

ρ_{M} (t_{0})

ρ_{M} (t)

ρ_{M} (t_{0})

order

ρ_{M} (t)

ρ_{M} (t_{0})

S_{0}

scale parameter

S_{0}^{'}

S_{0}

scale parameter

S_{0}^{'}

S_{0}

scale parameter

S_{0}^{'}

vacuum expectation value

G_{F}

Fermi’s

G_{e f f}

small, negative

G_{F}

Fermi’s

G_{e f f}

G_{F}

Fermi’s

G_{e f f}

G_{F}

Fermi’s

G_{e f f}

G_{F}

Fermi’s

G_{e f f}

G_{F}

Fermi’s

G_{e f f}

G_{F}

Fermi’s

G_{e f f}

G_{F}

Fermi’s

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G_{F}

Fermi’s

G_{e f f}

G_{F}

Fermi’s

G_{e f f}

G_{F}

Fermi’s

G_{e f f}

G_{F}

Fermi’s

G_{e f f}

G_{F}

Fermi’s

G_{e f f}

the cosmological

G_{F}

Fermi’s

G_{e f f}

a small, negative

G_{F}

Fermi’s

G_{e f f}

an appropriate

G_{F}

Fermi’s

G_{e f f}

ρ_{M} (t) = B / R^{3} (t)

ρ_{M} (t_{0})

ρ_{M} (t) = B / R^{3} (t)

ρ_{M} (t_{0})

ρ_{M} (t) = B / R^{3} (t)

t_{0}

age

ρ_{M} (t) = B / R^{3} (t)

ρ_{M} (t_{0})

ρ_{M} (t) = B / R^{3} (t)

ρ_{M} (t_{0})

order

ρ_{M} (t) = B / R^{3} (t)

ρ_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

future

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0

Ω_{Λ} (t)

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}^{'}

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

urfeld

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

field

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}^{'}

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

larger

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}^{'}

vacuum expectation value

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

a large rather than a small

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

scale parameter

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

a constant value

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

non-zero

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

S_{μ}^{μ} + S R_{μ}^{μ} / 6 = 0

field equation

S_{0}

background field

T^{μ ν}

T_{V}

a large

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{V}

big or small

T^{μ ν}

T_{V}

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{k i n}^{μ ν}

T^{μ ν}

T_{V}

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{V}

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{V}

T^{μ ν}

T_{V}

(highest) critical temperature

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{V}

T^{μ ν}

T_{V}

T^{μ ν}

T_{m a x}

T^{μ ν}

T_{V}

T^{μ ν}

T_{V}

T^{μ ν}

T_{m a x}

the temperature

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t)

t_{0}

age

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{k} (t)

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

negative

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

control

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

future

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

G_{e f f}

G_{F}

Fermi’s

λ S^{4}

S_{0}^{'}

λ S^{4}

S_{0}

λ S^{4}

S_{0}

urfeld

λ S^{4}

S_{0}

field

λ S^{4}

S_{0}

λ S^{4}

S_{0}^{'}

λ S^{4}

S_{0}

larger

λ S^{4}

S_{0}^{'}

vacuum expectation value

λ S^{4}

S_{0}

λ S^{4}

S_{0}

a large rather than a small

λ S^{4}

S_{0}

scale parameter

λ S^{4}

S_{0}

a constant value

λ S^{4}

S_{0}

non-zero

λ S^{4}

S_{0}

λ S^{4}

S_{0}

λ S^{4}

S_{0}

background field

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{V}

a large

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{m a x}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}^{'}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

small, negative

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{V}

big or small

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{V}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

urfeld

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

field

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

L_{P L}^{- 1}

inverse Planck length

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}^{'}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{m a x}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{m a x}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{k i n}^{μ ν}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{V}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{m a x}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T^{μ ν}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{m a x}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{V}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T^{μ ν}

the associated energy-momentum tensor

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

larger

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{m a x}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{V}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{V}

(highest) critical temperature

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}^{'}

vacuum expectation value

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{m a x}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

a large rather than a small

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

scale parameter

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{F}

Fermi’s

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T^{μ ν}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

L_{P L}^{- 1}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

a constant value

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{m a x}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

the cosmological

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{V}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

V_{m i n}^{G L}

which

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

non-zero

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

a small, negative

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{V}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

an appropriate

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{m a x}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{V}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{V}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

G_{e f f}

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

T_{m a x}

the temperature

V_{G L} (S, T) = g S^{4} - 2 g (T_{V}^{2} - T^{2}) S^{2}

effective Ginzburg-Landau potential

S_{0}

background field

S_{0}

a constant value

S_{0}^{'}

S_{0}

a constant value

S_{0}^{'}

S_{0}

a constant value

S_{0}^{'}

vacuum expectation value

S (x)

field

S_{0}^{'}

S (x)

field

S_{0}

S (x)

field

S_{0}

urfeld

S (x)

field

S_{0}

field

S (x)

field

S_{0}

S (x)

field

S_{0}^{'}

S (x)

field

S_{0}

larger

S (x)

field

S_{0}^{'}

vacuum expectation value

S (x)

field

S_{0}

S (x)

field

S_{0}

a large rather than a small

S (x)

field

S_{0}

scale parameter

S (x)

field

S_{0}

a constant value

S (x)

field

S_{0}

non-zero

S (x)

field

S_{0}

S (x)

field

S_{0}

S (x)

field

S_{0}

background field

T_{m a x} ≫ T (t_{0})

T_{V}

a large

T_{m a x} ≫ T (t_{0})

T_{V} ≫ T (t_{0})

T_{m a x} ≫ T (t_{0})

T_{V}

big or small

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T (t)

T_{m a x} ≫ T (t_{0})

T_{V} ≫ T (t_{0})

T_{m a x} ≫ T (t_{0})

T_{k i n}^{μ ν}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T^{μ ν}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T^{μ ν}

the associated energy-momentum tensor

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T_{V}

(highest) critical temperature

T_{m a x} ≫ T (t_{0})

T^{μ ν}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T_{V}

T_{m a x} ≫ T (t_{0})

T_{V}

d_{L} = c H {(t_{0})}^{- 1} 2 (1 + z) [1 - {(1 + z)}^{- 1 / 2}]

the (too bright for the data)

L_{P L}^{- 1}

inverse Planck length

d_{L} = c H {(t_{0})}^{- 1} 2 (1 + z) [1 - {(1 + z)}^{- 1 / 2}]

the (too bright for the data)

L_{P L}^{- 1}

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{V}

a large

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{m a x}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{V}

big or small

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{V}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{m a x}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{m a x}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{k i n}^{μ ν}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{V}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{m a x}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T^{μ ν}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{m a x}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{V}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T^{μ ν}

the associated energy-momentum tensor

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{m a x}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{V}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{V}

(highest) critical temperature

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{m a x}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T^{μ ν}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{m a x}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{V}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{V}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{m a x}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{V}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{V}

\nabla^{4} g_{00} = 3 (T_{0}^{0} - T_{r}^{r}) / 4 α_{g} g_{00} \equiv - f (r)

equation

T_{m a x}

the temperature

α > 0, k < 0

α_{g}

constant

α > 0, k < 0

α_{g}

constant

α > 0, k < 0

α_{g}

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

10^{- 2}

order

10^{- 60}

order

10^{- 2}

order

10^{60}

order

T (t_{0})

T_{V}

a large

T (t_{0})

T_{m a x}

T (t_{0})

T_{V}

big or small

T (t_{0})

T_{V}

T (t_{0})

T (t)

T (t_{0})

T_{m a x}

T (t_{0})

T_{m a x}

T (t_{0})

T_{k i n}^{μ ν}

T (t_{0})

T_{V}

T (t_{0})

T_{m a x}

T (t_{0})

T^{μ ν}

T (t_{0})

T_{m a x}

T (t_{0})

T_{V}

T (t_{0})

T^{μ ν}

the associated energy-momentum tensor

T (t_{0})

T_{m a x}

T (t_{0})

T_{V}

T (t_{0})

T_{V}

(highest) critical temperature

T (t_{0})

T_{m a x}

T (t_{0})

T^{μ ν}

T (t_{0})

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T (t_{0})

T_{m a x}

T (t_{0})

T_{V}

T (t_{0})

T_{V}

T (t_{0})

T_{m a x}

T (t_{0})

T_{V}

T (t_{0})

T_{V}

T (t_{0})

T_{m a x}

the temperature

β

β^{*}

G

an effective negative cosmological

G_{e f f}

small, negative

G

an effective negative cosmological

G_{e f f}

G

an effective negative cosmological

G_{e f f}

G

an effective negative cosmological

G_{e f f}

G

an effective negative cosmological

G_{e f f}

G

an effective negative cosmological

G_{e f f}

G

an effective negative cosmological

G_{e f f}

G

an effective negative cosmological

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

an effective negative cosmological

G_{e f f}

G

an effective negative cosmological

G_{e f f}

G

an effective negative cosmological

G_{e f f}

G

an effective negative cosmological

G_{F}

Fermi’s

G

an effective negative cosmological

G_{e f f}

G

an effective negative cosmological

G_{e f f}

the cosmological

G

an effective negative cosmological

G_{e f f}

a small, negative

G

an effective negative cosmological

G_{e f f}

an appropriate

G

an effective negative cosmological

G_{e f f}

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

q (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{k} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{M} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

the current era

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

q_{0}

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{M} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

q (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

q (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{M} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

t_{0}

age

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

the current era

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t)

future

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

the standard model

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

q_{0}

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

q (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

the current era

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t)

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

q (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{M} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{k} (t_{0})

orders

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

q (t_{0})

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

era

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

- q (t) = Ω_{Λ} (t) = 1 - Ω_{k} (t)

Ω_{Λ} (t_{0})

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t)

t_{0}

age

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

a large

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

big or small

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{k i n}^{μ ν}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T^{μ ν}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

(highest) critical temperature

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T^{μ ν}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

T_{V}

a large

T_{m a x}

T_{V}

big or small

T_{m a x}

T_{V}

T_{m a x}

T_{k i n}^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T_{V}

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

q (t_{0}) = - 0.37

q_{0}

q (t_{0}) = - 0.37

q (t)

conformal cosmology

q (t_{0}) = - 0.37

q (t)

q (t_{0}) = - 0.37

q_{0}

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{k} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

negative

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

control

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t)

future

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t)

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t)

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t_{0}) \approx 0

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) \approx 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{k} (t)

Ω_{M} (t_{0}) = 1

Ω_{k} (t_{0})

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{M} (t)

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0}) = 1

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 1

Ω_{M} (t)

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

negative

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

control

Ω_{M} (t_{0}) = 1

Ω_{M} (t)

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 1

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0}) = 1

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{M} (t)

Ω_{M} (t_{0}) = 1

Ω_{M} (t)

future

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{M} (t)

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{M} (t)

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{M} (t)

Ω_{M} (t_{0}) = 1

Ω_{M} (t)

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0}) = 1

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 1

Ω_{Λ} (t)

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{V}

a large

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{m a x}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}^{'}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{V}

big or small

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{V}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

urfeld

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

field

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}^{'}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{m a x}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{m a x}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{k i n}^{μ ν}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{V}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{m a x}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T^{μ ν}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{m a x}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{V}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T^{μ ν}

the associated energy-momentum tensor

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

larger

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{m a x}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{V}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{V}

(highest) critical temperature

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}^{'}

vacuum expectation value

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{m a x}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

a large rather than a small

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

scale parameter

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T^{μ ν}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

a constant value

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{m a x}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{V}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

V_{m i n}^{G L}

which

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

non-zero

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{V}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{m a x}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{V}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{V}

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

T_{m a x}

the temperature

- c Λ = - c ℏ λ^{'} S_{0}^{', 4} = σ T_{V}^{4}

S_{0}

background field

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

t a n h^{2} (3 D^{1 / 2} t / 2)

t_{0}

age

G_{e f f}

the cosmological

G_{F}

Fermi’s

q (t_{0})

q_{0}

q (t_{0})

q (t)

conformal cosmology

q (t_{0})

q (t)

q (t_{0})

q_{0}

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

t_{0}

age

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

α > 0, k > 0

α_{g}

constant

α > 0, k > 0

α_{g}

constant

α > 0, k > 0

α_{g}

q (t) \sim - 1

q (t_{0})

q (t) \sim - 1

q_{0}

q (t) \sim - 1

q (t_{0})

q (t) \sim - 1

q (t_{0})

q (t) \sim - 1

t_{0}

age

q (t) \sim - 1

q_{0}

q (t) \sim - 1

q (t_{0})

q (t) \sim - 1

q (t_{0})

q (t) \sim - 1

q (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{k} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{k} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

future

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{M} (t_{0})

Ω_{Λ} (t_{0}) = 0.7

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0}) = 0.7

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = 0.7

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t)

t_{0}

age

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{k} (t)

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

negative

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

control

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

future

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

Ω_{M} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0}) ≃ Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{k} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{k} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{M} (t)

future

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

line

Ω_{Λ} (t)

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}^{'}

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

urfeld

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

field

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}^{'}

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

larger

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}^{'}

vacuum expectation value

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

a large rather than a small

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

scale parameter

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

λ S^{4}

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

a constant value

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

λ S^{4}

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

non-zero

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

λ = λ^{'} S_{0}^{', 4} / S_{0}^{4} ≪ λ^{'}

S_{0}

background field

T_{V}^{4} / T^{4}

T_{V}

a large

T_{V}^{4} / T^{4}

T_{m a x}

T_{V}^{4} / T^{4}

T_{V}

big or small

T_{V}^{4} / T^{4}

T_{V}

T_{V}^{4} / T^{4}

T_{m a x} / T_{V}

such a choice

T_{V}^{4} / T^{4}

T_{m a x}

T_{V}^{4} / T^{4}

T_{m a x}

T_{V}^{4} / T^{4}

T^{4} / T_{V}^{4}

T_{V}^{4} / T^{4}

T_{k i n}^{μ ν}

T_{V}^{4} / T^{4}

T_{V}

T_{V}^{4} / T^{4}

T_{m a x}

T_{V}^{4} / T^{4}

T^{μ ν}

T_{V}^{4} / T^{4}

T_{m a x}

T_{V}^{4} / T^{4}

T_{V}

T_{V}^{4} / T^{4}

T^{μ ν}

the associated energy-momentum tensor

T_{V}^{4} / T^{4}

T_{m a x}

T_{V}^{4} / T^{4}

T_{V}

T_{V}^{4} / T^{4}

T_{V}

(highest) critical temperature

T_{V}^{4} / T^{4}

T_{m a x}

T_{V}^{4} / T^{4}

T^{μ ν}

T_{V}^{4} / T^{4}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}^{4} / T^{4}

T_{m a x}

T_{V}^{4} / T^{4}

T_{V}

T_{V}^{4} / T^{4}

V_{m i n}^{G L}

which

T_{V}^{4} / T^{4}

T_{V}

T_{V}^{4} / T^{4}

T_{m a x}

T_{V}^{4} / T^{4}

T_{V}

T_{V}^{4} / T^{4}

T_{V}

T_{V}^{4} / T^{4}

T_{m a x}

the temperature

ρ_{M} (t_{0})

order

ρ_{M} (t)

perfectly normal

ρ_{M} (t_{0})

order

ρ_{M} (t)

ρ_{M} (t_{0})

order

ρ_{M} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

q (t) = (n / 2 - 1) Ω_{M} (t) - Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{k} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

q_{0}

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

q (t)

conformal cosmology

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

q (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t)

future

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

q_{0}

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

q (t_{0}) = (n / 2 - 1) Ω_{M} (t_{0}) - Ω_{Λ} (t_{0})

Ω_{Λ} (t)

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{k} (t)

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

future

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

negative

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

control

Ω_{M} (t)

t_{0}

age

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t)

β^{*} = \int d r f (r) r^{4} / 12

d_{L}

- 2 λ^{'} S_{0}^{', 2}

S_{0}^{'}

- 2 λ^{'} S_{0}^{', 2}

S_{0}

- 2 λ^{'} S_{0}^{', 2}

S_{0}

urfeld

- 2 λ^{'} S_{0}^{', 2}

S_{0}

field

- 2 λ^{'} S_{0}^{', 2}

S_{0}

- 2 λ^{'} S_{0}^{', 2}

S_{0}^{'}

- 2 λ^{'} S_{0}^{', 2}

S_{0}

larger

- 2 λ^{'} S_{0}^{', 2}

S_{0}^{'}

vacuum expectation value

- 2 λ^{'} S_{0}^{', 2}

S_{0}

- 2 λ^{'} S_{0}^{', 2}

S_{0}

a large rather than a small

- 2 λ^{'} S_{0}^{', 2}

S_{0}

scale parameter

- 2 λ^{'} S_{0}^{', 2}

S_{0}

a constant value

- 2 λ^{'} S_{0}^{', 2}

S_{0}

non-zero

- 2 λ^{'} S_{0}^{', 2}

S_{0}

- 2 λ^{'} S_{0}^{', 2}

S_{0}

- 2 λ^{'} S_{0}^{', 2}

S_{0}

background field

\dot{R} (t = 0)

t_{0}

age

q (t_{0}) = 0

q_{0}

q (t_{0}) = 0

q (t)

conformal cosmology

q (t_{0}) = 0

q (t)

q (t_{0}) = 0

q_{0}

R (t) = {(B / c Λ)}^{1 / 3} s i n h^{2 / 3} (3 D^{1 / 2} t / 2)

t_{0}

age

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{k i n}^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

T_{V}

V_{m i n}^{G L}

which

T_{V}

T_{m a x}

T_{V}

T_{m a x}

the temperature

G

the standard attractive

G_{e f f}

small, negative

G

the standard attractive

G_{e f f}

G

the standard attractive

G_{e f f}

G

the standard attractive

G_{e f f}

G

the standard attractive

G_{e f f}

G

the standard attractive

G_{e f f}

G

the standard attractive

G_{e f f}

G

the standard attractive

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

the standard attractive

G_{e f f}

G

the standard attractive

G_{e f f}

G

the standard attractive

G_{e f f}

G

the standard attractive

G_{F}

Fermi’s

G

the standard attractive

G_{e f f}

G

the standard attractive

G_{e f f}

the cosmological

G

the standard attractive

G_{e f f}

a small, negative

G

the standard attractive

G_{e f f}

an appropriate

G

the standard attractive

G_{e f f}

ρ_{M} (t_{0})

ρ_{M} (t)

perfectly normal

ρ_{M} (t_{0})

ρ_{M} (t)

ρ_{M} (t_{0})

ρ_{M} (t)

V_{m i n}^{G L}

which

G_{e f f}

small, negative

V_{m i n}^{G L}

which

G_{e f f}

V_{m i n}^{G L}

which

G_{e f f}

V_{m i n}^{G L}

which

L_{P L}^{- 1}

inverse Planck length

V_{m i n}^{G L}

which

G_{e f f}

V_{m i n}^{G L}

which

G_{e f f}

V_{m i n}^{G L}

which

G_{e f f}

V_{m i n}^{G L}

which

G_{e f f}

V_{m i n}^{G L}

which

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

V_{m i n}^{G L}

which

G_{e f f}

V_{m i n}^{G L}

which

G_{e f f}

V_{m i n}^{G L}

which

G_{e f f}

V_{m i n}^{G L}

which

G_{F}

Fermi’s

V_{m i n}^{G L}

which

G_{e f f}

V_{m i n}^{G L}

which

L_{P L}^{- 1}

V_{m i n}^{G L}

which

G_{e f f}

the cosmological

V_{m i n}^{G L}

which

G_{e f f}

a small, negative

V_{m i n}^{G L}

which

G_{e f f}

an appropriate

V_{m i n}^{G L}

which

G_{e f f}

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}^{'}

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

urfeld

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

field

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}^{'}

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

larger

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}^{'}

vacuum expectation value

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

a large rather than a small

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

scale parameter

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

a constant value

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

non-zero

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

- 3 c^{3} / 4 π ℏ S_{0}^{2}

S_{0}

background field

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

small, negative

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

Λ ≃ V_{m i n}^{G L}

effective

L_{P L}^{- 1}

inverse Planck length

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

Λ ≃ V_{m i n}^{G L}

effective

G_{F}

Fermi’s

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

Λ ≃ V_{m i n}^{G L}

effective

L_{P L}^{- 1}

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

the cosmological

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

a small, negative

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

an appropriate

Λ ≃ V_{m i n}^{G L}

effective

G_{e f f}

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{k} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{k} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

negative

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

control

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

future

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{M} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0}) = 0.3

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) = 0.3

Ω_{Λ} (t)

α > 0

α_{g}

constant

α > 0

α_{g}

constant

α > 0

α_{g}

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

G

the standard

G_{e f f}

small, negative

G

the standard

G_{e f f}

G

the standard

G_{e f f}

G

the standard

G_{e f f}

G

the standard

G_{e f f}

G

the standard

G_{e f f}

G

the standard

G_{e f f}

G

the standard

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

the standard

G_{e f f}

G

the standard

G_{e f f}

G

the standard

G_{e f f}

G

the standard

G_{F}

Fermi’s

G

the standard

G_{e f f}

G

the standard

G_{e f f}

the cosmological

G

the standard

G_{e f f}

a small, negative

G

the standard

G_{e f f}

an appropriate

G

the standard

G_{e f f}

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

t_{0}

age

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

R (t) = {(- B / c Λ)}^{1 / 3} c o s h^{2 / 3} (3 D^{1 / 2} t / 2)

t_{0}

age

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{V}

a large

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{V}

big or small

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{V}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{m a x} / T_{V}

such a choice

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T^{4} / T_{V}^{4}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{k i n}^{μ ν}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

β^{*}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{V}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T^{μ ν}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{V}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T^{μ ν}

the associated energy-momentum tensor

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{V}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{V}

(highest) critical temperature

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T^{μ ν}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{V}^{4} / T^{4}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{V}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

V_{m i n}^{G L}

which

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{V}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{V}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{V}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

T_{m a x}

the temperature

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

λ S^{4}

S_{0}^{'}

λ S^{4}

S_{0}

λ S^{4}

S_{0}

urfeld

λ S^{4}

S_{0}

field

λ S^{4}

S_{0}

λ S^{4}

S_{0}^{'}

λ S^{4}

S_{0}

larger

λ S^{4}

S_{0}^{'}

vacuum expectation value

λ S^{4}

S_{0}

λ S^{4}

S_{0}

a large rather than a small

λ S^{4}

S_{0}

scale parameter

λ S^{4}

S_{0}

a constant value

λ S^{4}

S_{0}

non-zero

λ S^{4}

S_{0}

λ S^{4}

S_{0}

λ S^{4}

S_{0}

background field

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{k} (t)

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

t_{0}

age

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t)

future

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t) / {\bar{Ω}}_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t)

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t) / Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t) / Ω_{M} (t)

Ω_{Λ} (t_{0})

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{V}

a large

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{V}

big or small

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{V}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{m a x} / T_{V}

such a choice

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T^{4} / T_{V}^{4}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{k i n}^{μ ν}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

β^{*}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{V}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T^{μ ν}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{V}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T^{μ ν}

the associated energy-momentum tensor

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{V}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{V}

(highest) critical temperature

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T^{μ ν}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{V}^{4} / T^{4}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{V}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

V_{m i n}^{G L}

which

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

(β - 1) / (β + 1) = T_{V}^{4} / T_{m a x}^{4}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{V}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{m a x}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{V}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{V}

(β - 1) / (β + 1) = T_{m a x}^{4} / T_{V}^{4}

T_{m a x}

the temperature

α > 0

α_{g}

constant

α > 0

α_{g}

constant

α > 0

α_{g}

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{Λ} (t)

S_{0}

non-zero

S_{0}^{'}

S_{0}

non-zero

S_{0}^{'}

S_{0}

non-zero

S_{0}^{'}

vacuum expectation value

\dot{R} (t = 0)

overwhelmingly large

t_{0}

age

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t)

t_{0}

age

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

G_{e f f}

a small, negative

G_{F}

Fermi’s

G

the effective

G_{e f f}

small, negative

G

the effective

G_{e f f}

G

the effective

G_{e f f}

G

the effective

G_{e f f}

G

the effective

G_{e f f}

G

the effective

G_{e f f}

G

the effective

G_{e f f}

G

the effective

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

the effective

G_{e f f}

G

the effective

G_{e f f}

G

the effective

G_{e f f}

G

the effective

G_{F}

Fermi’s

G

the effective

G_{e f f}

G

the effective

G_{e f f}

the cosmological

G

the effective

G_{e f f}

a small, negative

G

the effective

G_{e f f}

an appropriate

G

the effective

G_{e f f}

{\bar{Ω}}_{M} (t = 0)

{\bar{Ω}}_{Λ} (t = 0)

{\bar{Ω}}_{M} (t = 0)

t_{0}

age

{\bar{Ω}}_{M} (t = 0)

Ω_{M} (t = 0)

initial

{\bar{Ω}}_{M} (t = 0)

Ω_{Λ} (t = 0)

initial

T_{V} \geq T_{m a x} ≫ T (t_{0})

T (t)

T_{V} \geq T_{m a x} ≫ T (t_{0})

T_{k i n}^{μ ν}

T_{V} \geq T_{m a x} ≫ T (t_{0})

T^{μ ν}

T_{V} \geq T_{m a x} ≫ T (t_{0})

T^{μ ν}

the associated energy-momentum tensor

T_{V} \geq T_{m a x} ≫ T (t_{0})

T^{μ ν}

T_{V} \geq T_{m a x} ≫ T (t_{0})

V_{m i n}^{G L}

which

q (t_{0})

q_{0}

q (t_{0})

q (t)

conformal cosmology

q (t_{0})

q (t)

q (t_{0})

q_{0}

β

β^{*}

R (t)

t_{0}

age

R (t) \sim t

t_{0}

age

S_{0}

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

S_{0}^{'}

vacuum expectation value

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

α

matter how large

α_{g}

constant

α

matter how large

α_{g}

constant

α

matter how large

α_{g}

10^{60}

order

10^{- 60}

order

10^{60}

order

10^{- 2}

order

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{k i n}^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

T_{V}

V_{m i n}^{G L}

which

T_{V}

T_{m a x}

T_{V}

T_{m a x}

the temperature

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

I_{W}

purely gravitational piece

W^{μ ν}

I_{W}

purely gravitational piece

W^{μ ν}

I_{W}

purely gravitational piece

W^{μ ν}

__TABLE_2__

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

- 10^{120}

10^{- 60}

order

- 10^{120}

- 10^{60}

order

- 10^{120}

10^{- 2}

order

- 10^{120}

10^{60}

order

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

α

parameter

α_{g}

constant

α

parameter

α_{g}

constant

α

parameter

α_{g}

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t, α > 0, k < 0)

spatial 3-curvature

t_{0}

age

Ω_{Λ} (t, α > 0, k < 0)

spatial 3-curvature

α_{g}

constant

Ω_{Λ} (t, α > 0, k < 0)

spatial 3-curvature

α_{g}

constant

Ω_{Λ} (t, α > 0, k < 0)

spatial 3-curvature

α_{g}

ρ_{M} (t)

ρ_{M} (t_{0})

ρ_{M} (t)

ρ_{M} (t_{0})

ρ_{M} (t)

t_{0}

age

ρ_{M} (t)

ρ_{M} (t_{0})

ρ_{M} (t)

ρ_{M} (t_{0})

order

ρ_{M} (t)

ρ_{M} (t_{0})

T^{μ ν} = 0

motion

T_{V}

a large

T^{μ ν} = 0

motion

T_{m a x}

T^{μ ν} = 0

motion

T_{V}

big or small

T^{μ ν} = 0

motion

T_{V}

T^{μ ν} = 0

motion

T_{m a x}

T^{μ ν} = 0

motion

T_{m a x}

T^{μ ν} = 0

motion

T_{k i n}^{μ ν}

T^{μ ν} = 0

motion

T_{V}

T^{μ ν} = 0

motion

T_{m a x}

T^{μ ν} = 0

motion

T_{m a x}

T^{μ ν} = 0

motion

T_{V}

T^{μ ν} = 0

motion

T_{m a x}

T^{μ ν} = 0

motion

T_{V}

T^{μ ν} = 0

motion

T_{V}

(highest) critical temperature

T^{μ ν} = 0

motion

T_{k i n}^{μ ν} = 0

T^{μ ν} = 0

motion

T_{m a x}

T^{μ ν} = 0

motion

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T^{μ ν} = 0

motion

T_{m a x}

T^{μ ν} = 0

motion

T_{V}

T^{μ ν} = 0

motion

T_{V}

T^{μ ν} = 0

motion

T_{m a x}

T^{μ ν} = 0

motion

T_{V}

T^{μ ν} = 0

motion

T_{V}

T^{μ ν} = 0

motion

T_{m a x}

the temperature

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{k} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{k} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{M} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{M} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

negative

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

control

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{M} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{M} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{M} (t)

future

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{M} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{M} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{M} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{M} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t_{0})

Ω_{M} (t_{0}) \approx 0.3

currently preferred standard model

Ω_{Λ} (t)

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}^{'}

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

urfeld

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

field

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}^{'}

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

larger

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}^{'}

vacuum expectation value

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

a large rather than a small

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

scale parameter

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

a constant value

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

non-zero

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

Λ = ℏ λ S_{0}^{4}

a large rather than a small

S_{0}

background field

q (t_{0}) = (n / 2 - 1) (1 + k c^{2} / {\dot{R}}^{2} (t_{0})) - n {\bar{Ω}}_{Λ} (t_{0}) / 2)

q_{0}

q (t_{0}) = (n / 2 - 1) (1 + k c^{2} / {\dot{R}}^{2} (t_{0})) - n {\bar{Ω}}_{Λ} (t_{0}) / 2)

q_{0}

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

S_{0}

S_{0}^{'}

S_{0}

S_{0}^{'}

S_{0}

S_{0}^{'}

vacuum expectation value

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t)

Ω_{M} (t_{0})

Ω_{k} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

negative

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

control

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

future

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

the standard model

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

Ω_{M} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

G_{e f f}

an appropriate

G_{F}

Fermi’s

T_{m a x}

T_{V}

a large

T_{m a x}

T_{V}

big or small

T_{m a x}

T_{V}

T_{m a x}

T_{k i n}^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

T_{V}

T_{m a x}

T_{V}

(highest) critical temperature

T_{m a x}

T^{μ ν}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{k} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

negative

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

control

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t)

future

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0})

orders

Ω_{M} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{M} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

Ω_{Λ} (t, α > 0)

t_{0}

age

Ω_{Λ} (t, α > 0)

α_{g}

constant

Ω_{Λ} (t, α > 0)

α_{g}

constant

Ω_{Λ} (t, α > 0)

α_{g}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{k i n}^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

T_{V}

V_{m i n}^{G L}

which

T_{V}

T_{m a x}

T_{V}

T_{m a x}

the temperature

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{k} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0}) = 1

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

negative

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

control

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

future

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0}) = 1

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) = 1

Ω_{M} (t)

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t_{0}) = 1

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 1

Ω_{Λ} (t)

q (t_{0})

q_{0}

q (t_{0})

q (t)

conformal cosmology

q (t_{0})

q (t)

q (t_{0})

q_{0}

q (k = 0, t_{0}) = 1 / 2

q_{0}

q (k = 0, t_{0}) = 1 / 2

q_{0}

Ω_{M} (t = 0)

initial

{\bar{Ω}}_{M} (t = 0)

universe

Ω_{M} (t = 0)

initial

{\bar{Ω}}_{Λ} (t = 0)

Ω_{M} (t = 0)

initial

t_{0}

age

Ω_{M} (t = 0)

initial

{\bar{Ω}}_{M} (t = 0)

Ω_{M} (t = 0)

initial

Ω_{Λ} (t = 0)

initial

α < 0

α_{g}

constant

α < 0

α_{g}

constant

α < 0

α_{g}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T_{k i n}^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

the associated energy-momentum tensor

T_{V}

T_{m a x}

T_{V}

T_{m a x}

T_{V}

T^{μ ν}

T_{V}

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

T_{V}

T_{m a x}

T_{V}

V_{m i n}^{G L}

which

T_{V}

T_{m a x}

T_{V}

T_{m a x}

the temperature

G_{e f f}

G_{F}

Fermi’s

{\bar{Ω}}_{Λ} (t) H^{2} (t)

The quantity

t_{0}

age

T_{m a x}

the temperature

T_{V}

a large

T_{m a x}

the temperature

T_{V}

big or small

T_{m a x}

the temperature

T_{V}

T_{m a x}

the temperature

T_{k i n}^{μ ν}

T_{m a x}

the temperature

T_{V}

T_{m a x}

the temperature

T^{μ ν}

T_{m a x}

the temperature

T_{V}

T_{m a x}

the temperature

T^{μ ν}

the associated energy-momentum tensor

T_{m a x}

the temperature

T_{V}

T_{m a x}

the temperature

T_{V}

(highest) critical temperature

T_{m a x}

the temperature

T^{μ ν}

T_{m a x}

the temperature

T_{V}

T_{m a x}

the temperature

T_{V}

T_{m a x}

the temperature

T_{V}

T_{m a x}

the temperature

T_{V}

Ω_{M} (t = 0) + Ω_{Λ} (t = 0) = 1

t_{0}

age

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

t_{0}

age

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

the rather tight

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{k} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

negative

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

control

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

future

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

the standard model

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0}) = 0

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

the current era

Ω_{k} (t_{0}) = 0

Ω_{M} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0}) = 0

viz.

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{M} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t_{0}) = 0

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t_{0})

Ω_{k} (t_{0}) = 0

Ω_{Λ} (t)

3.06 \times 10^{- 30}

10^{- 60}

order

3.06 \times 10^{- 30}

10^{- 2}

order

3.06 \times 10^{- 30}

10^{60}

order

S_{0}

background field

S_{0}^{'}

S_{0}

background field

S_{0}^{'}

S_{0}

background field

S_{0}^{'}

vacuum expectation value

d s^{2} = (1 + γ_{0} r) c^{2} d t^{2} - d r^{2} / (1 + γ_{0} r) - r^{2} d Ω

metric

t_{0}

age

d s^{2} = (1 + γ_{0} r) c^{2} d t^{2} - d r^{2} / (1 + γ_{0} r) - r^{2} d Ω

metric

d_{L}

G

G_{e f f}

small, negative

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem

G

G_{e f f}

G

G_{e f f}

G

G_{e f f}

G

G_{F}

Fermi’s

G

G_{e f f}

G

G_{e f f}

the cosmological

G

G_{e f f}

a small, negative

G

G_{e f f}

an appropriate

G

G_{e f f}

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

negative

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

control

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

the quantity

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

future

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{M} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{k} (t)

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{k} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{M} (t)

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t)

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

the current era

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{M} (t)

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{M} (t)

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t)

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

t_{0}

age

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t)

0 \leq Ω_{Λ} (t) \leq 1

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

the quantity

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

the current era

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

the quantity

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

the same order of magnitude

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

0 \leq {\bar{Ω}}_{Λ} (t_{0}) \leq 1

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t)

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t)

future

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t)

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t)

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

the standard model

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t)

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t)

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

the current era

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t)

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t)

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{M} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

0 \leq Ω_{Λ} (t) \leq 1

Ω_{k} (t_{0})

orders

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{M} (t_{0})

era

0 \leq Ω_{Λ} (t) \leq 1

{\bar{Ω}}_{Λ} (t_{0})

the current era

0 \leq Ω_{Λ} (t) \leq 1

Ω_{Λ} (t_{0})

q (t_{0}) = - 1 / 2

q_{0}

q (t_{0}) = - 1 / 2

q (t)

conformal cosmology

q (t_{0}) = - 1 / 2

q (t)

q (t_{0}) = - 1 / 2

q_{0}

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

negative

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

control

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

the same order of magnitude

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

future

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

the standard model

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{M} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{k} (t_{0})

orders

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

{\bar{Ω}}_{M} (t_{0})

era

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{V}

a large

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{m a x}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{V}

big or small

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{V}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{m a x}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{m a x}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{k i n}^{μ ν}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{V}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{m a x}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T^{μ ν}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{m a x}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{V}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T^{μ ν}

the associated energy-momentum tensor

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{m a x}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{V}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{V}

(highest) critical temperature

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{m a x}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T^{μ ν}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{m a x}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{V}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

V_{m i n}^{G L}

which

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{V}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{m a x}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{V}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{V}

{(1 + T^{2} T_{m a x}^{2} / T_{V}^{4})}^{- 1}

the quantity

T_{m a x}

the temperature

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{k} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{k} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

t_{0}

age

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t)

future

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{M} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{k} (t_{0})

orders

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t) = t a n h^{2} (3 D^{1 / 2} t / 2)

dependence

Ω_{Λ} (t_{0})

- q (t) H^{2} (t)

q_{0}

- q (t) H^{2} (t)

t_{0}

age

- q (t) H^{2} (t)

q_{0}

Ω_{Λ} (t, α > 0, k < 0)

t_{0}

age

Ω_{Λ} (t, α > 0, k < 0)

α_{g}

constant

Ω_{Λ} (t, α > 0, k < 0)

α_{g}

constant

Ω_{Λ} (t, α > 0, k < 0)

α_{g}

Ω_{Λ} (t = 0)

initial

{\bar{Ω}}_{M} (t = 0)

universe

Ω_{Λ} (t = 0)

initial

{\bar{Ω}}_{Λ} (t = 0)

Ω_{Λ} (t = 0)

initial

t_{0}

age

Ω_{Λ} (t = 0)

initial

{\bar{Ω}}_{M} (t = 0)

Ω_{Λ} (t = 0)

initial

Ω_{M} (t = 0)

initial

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

t_{0}

age

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

future

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{M} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{M} (t_{0})

Ω_{Λ} (t_{0})

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0})

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{V}

a large

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

q (t_{0})

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{m a x}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{V}

big or small

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{V}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{m a x} / T_{V}

such a choice

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

q_{0}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{m a x}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{m a x}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T^{4} / T_{V}^{4}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

q (t_{0})

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

q (t_{0})

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{k i n}^{μ ν}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{V}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{m a x}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T^{μ ν}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{m a x}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{V}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T^{μ ν}

the associated energy-momentum tensor

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

t_{0}

age

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{m a x}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{V}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{V}

(highest) critical temperature

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{m a x}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T^{μ ν}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{m a x}

__TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{m a x}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

q_{0}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

q (t_{0})

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{V}^{4} / T^{4}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{V}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

q (t_{0})

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{V}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{m a x}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{V}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

q (t_{0})

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{V}

q (t) = {[1 - T_{m a x}^{2} / T^{2} (t)]}^{- 1}

(18

T_{m a x}

the temperature

d_{L}

L_{P L}^{- 1}

inverse Planck length

d_{L}

L_{P L}^{- 1}

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

t_{0}

age

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the same order of magnitude

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

future

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

the standard model

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

Ω_{M} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{M} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t)

Ω_{M} (t_{0})

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t)

Ω_{k} (t_{0})

orders

Ω_{Λ} (t)

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t)

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t)

Ω_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{k} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{k} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

negative

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

control

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

the quantity

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{M} (t)

future

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{M} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{M} (t_{0})

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{k} (t_{0})

orders

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{M} (t_{0})

era

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

{\bar{Ω}}_{Λ} (t_{0})

the current era

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

Ω_{Λ} (t_{0}) = Ω_{M} (t_{0}) + 1 / 2

Ω_{Λ} (t)

ρ_{M} (t) = A / R^{4}

ρ_{M} (t_{0})

ρ_{M} (t) = A / R^{4}

ρ_{M} (t_{0})

ρ_{M} (t) = A / R^{4}

t_{0}

age

ρ_{M} (t) = A / R^{4}

ρ_{M} (t_{0})

ρ_{M} (t) = A / R^{4}

ρ_{M} (t_{0})

order

ρ_{M} (t) = A / R^{4}

ρ_{M} (t_{0})